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simulation

Paper Title Other Keywords Page
MO3RAI01 A Few Issues on the Upgrade of KEKB B-Factory luminosity, factory, impedance, radiation 23
 
  • K. Oide, T. Abe, K. Akai, Y. Funakoshi, T. Kageyama, H. Koiso, K. Ohmi, Y. Ohnishi, K. Shibata, Y. Suetsugu, M. Tobiyama
    KEK, Ibaraki
 
 

A few issues on the path of the luminosity upgrade of KEKB B-Factory is described, including coherent synchrotron radiation, design of the interaction region, crab crossing, and high current operation. These issues will raise more obstacles on the upgrade with the High-Current Scheme. As an alternative, {¥it Nano-Beam Scheme} should be considered as a possible option for the upgrade.

 

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MO3RAC04 Super-B Project Overview sextupole, luminosity, emittance, lattice 38
 
  • M.E. Biagini, R. Boni, M. Boscolo, T. Demma, A. Drago, S. Guiducci, P. Raimondi, S. Tomassini, M. Zobov
    INFN/LNF, Frascati (Roma)
  • K.J. Bertsche, M.H. Donald, Y. Nosochkov, A. Novokhatski, J. Seeman, M.K. Sullivan, U. Wienands, W. Wittmer, G. Yocky
    SLAC, Menlo Park, California
  • S. Bettoni, D. Quatraro
    CERN, Geneva
  • I. Koop, E.B. Levichev, S.A. Nikitin, P.A. Piminov, D.N. Shatilov
    BINP SB RAS, Novosibirsk
  • K. Ohmi
    KEK, Ibaraki
  • E. Paoloni
    University of Pisa and INFN, Pisa
 
 

The SuperB project aims at the construction of an asymmetric (4x7 GeV), very high luminosity, B-Factory on the Roma II (Italy) University campus. The luminosity goal of 1036 cm-2 s-1 can be reached with a new collision scheme with large Piwinski angle and the use of “crab” sextupoles. A crab-waist IR has been successfully tested at the DAPHNE Phi-Factory at LNF-Frascati (Italy) in 2008. The crab waist together with very low beta* will allow for operation with relatively low beam currents and reasonable bunch length, comparable to those of PEP-II and KEKB. In the High Energy Ring, two spin rotators permit bringing longitudinally polarized beams into collision at the IP. The lattice has been designed with a very low intrinsic emittance and is quite compact, less than 2 km long. The tight focusing requires a sophisticated Interaction Region with quadrupoles very close to the IP. A Conceptual Design Report was published in March 2007, and beam dynamics and collective effects R&D studies are in progress in order to publish a Technical Design Report by the end of 2010. A status of the design and simulations is presented in this paper.

 

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MO3RAC05 Dynamic Beta/Emittance Effects in the Measurement of Horizontal Beam Sizes emittance, luminosity, synchrotron, radiation 41
 
  • K. Ohmi, J.W. Flanagan, Y. Funakoshi, K. Oide
    KEK, Ibaraki
  • Y. Cai
    SLAC, Menlo Park, California
 
 

It is well known that the beam-beam interaction has a focusing effect and therefore causes a dynamical beating of beta function around the rings. This effect becomes greatly enhanced when a collider, such as KEKB, is operated near half integer. The beating makes it difficult to interpret the measurement of horizontal beam size. We derived two coupled nonlinear equations and solved them analytically to obtain the beam sizes at the interaction points, taking into account of dynamical beta and emittance. It has been demonstrated its effectiveness using actual measured data at the synchrotron light monitors. It is expected that it will be implemented in the control room.

 

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MO4RAC02 Status of LHC Crab Cavity Simulations and Beam Studies cavity, luminosity, impedance, damping 85
 
  • R. Calaga, R. De Maria
    BNL, Upton, Long Island, New York
  • R.W. Assmann, J. Barranco, F. Caspers, E. Ciapala, T.P.R. Linnecar, E. Métral, Y. Sun, R. Tomás, J. Tuckmantel, Th. Weiler, F. Zimmermann
    CERN, Geneva
  • G. Burt
    Lancaster University, Lancaster
  • Y. Funakoshi, A. Morita, Y. Morita, K. Nakanishi, Y. Ohnishi
    KEK, Ibaraki
  • Z. Li, A. Seryi, L. Xiao
    SLAC, Menlo Park, California
  • P.A. McIntosh
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • J. Qiang
    LBNL, Berkeley, California
  • N. Solyak, V.P. Yakovlev
    Fermilab, Batavia
 
 

Funding: This work was partially performed under the auspices of the US DOE and the European Community-Research Infrastructure, FP6 programme (CARE, contract number RII3-CT-2003-506395)}


The LHC crab cavity program is advancing rapidly towards a first prototype which is anticipated to be tested during the early stages of the LHC phase I upgrade and commissioning. Some aspects related to crab optics, collimation, aperture constraints, impedances, noise effects, beam transparency and machine protection critical for a safe and robust operation of LHC beams with crab cavities are addressed here.

 

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MO4RAC05 Weak-Strong Simulation of Head-On Beam-Beam Compensation in the RHIC proton, electron, emittance, multipole 94
 
  • Y. Luo, R. De Maria, W. Fischer, N. Milas, G. Robert-Demolaize
    BNL, Upton, Long Island, New York
  • E. McIntosh
    CERN, Geneva
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy and the US LHC Accelerator Research Program (LARP).


In the Relativistic Heavy Ion Collider (RHIC) beams collide in the two interaction points IP6 and IP8. An increase of the bunch intensity above 2·1011 in polarized proton operation appears difficult due to the large beam-beam tune spread generated by the two collisions. A low energy electron beam or electron lens has been proposed to mitigate the head on beam-beam effect. In RHIC such a device could be located near IP10. We summarize multi-particle weak-strong beam-beam simulations of head-on beam-beam compensation with an electron lens. The proton beam's lifetime and emittance are calculated and compared for situations with and without an electron lens. Parameters such as the proton bunch intensity, the electron beam intensity and the betatron phase advances between IP8 and IP10 are scanned in the simulations.

 

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MO4GRI01 High Power Fast Ramping Power Supplies power-supply, controls, proton, heavy-ion 112
 
  • I. Marneris, E.M. Bajon, R. Bonati, T. Roser, J. Sandberg, N. Tsoupas
    BNL, Upton, Long Island, New York
 
 

Hundred megawatt level fast ramping power converters to drive proton and heavy ion machines are under research and development at accelerator facilities in the world. This is a leading edge technology. There are several topologies to achieve this power level. Their advantages and related issues will be discussed.

 

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MO6PFP004 Small Gap Magnets and Vacuum Chambers for eRHIC dipole, vacuum, electron, quadrupole 133
 
  • W. Meng, Y. Hao, A.K. Jain, V. Litvinenko, G.J. Mahler, J.E. Tuozzolo
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


eRHIC, a future high luminosity electron-ion collider at BNL, will add polarized electrons to the list of colliding species in RHIC. A 10-to-30 GeV electron energy recovery linac will require up to six passes around the RHIC 3.8 km circumference. We are developing and testing small (3-to-5 mm gap) dipole and quadrupole magnets and vacuum chambers for cost-effective eRHIC passes. We are also studying the sensitivity of eRHIC pass optics to magnet and alignment errors in such a small-magnet structure. We present the magnetic and mechanical designs of the small gap eRHIC components and prototyping test results.

 
MO6PFP011 Imperfection Investigation for the Main Magnet Construction for Compact Cyclotron cyclotron, cavity, controls, vacuum 154
 
  • T.J. Zhang, Y.L. Lu, C. Wang, S.M. Wei, J.J. Yang, H.J. Yao, J.Q. Zhong
    CIAE, Beijing
 
 

CYCIAE-100 is a 100 MeV, 200 muA H- cyclotron being constructed at CIAE. The tolerance of the magnetic field is as tight as 1.2 Gauss for isochronous field and 2 Gauss for first harmonics. Due to the absence of coil adjusting in this machine, a measure that helps to achieve a more compact structure (435 ton for the main magnet), the imperfection hence becomes a much more critical factor in our consideration. The effects by the various kinds of imperfection are investigated numerically and the imperfection fields are predicted for beam dynamics simulation, serving as a basic guidance in the magnet construction for CYCIAE-100. Some of the important results will be reported in this paper, including

  1. the deformation of the main magnet by the gravity itself, 480 ton EM force and 120 ton vacuum pressure,
  2. segregation, inclusion and contraction cavity induced by the casting procedure,
  3. fabrication and assembling tolerance, and
  4. thermal deformation.

 
MO6PFP031 3D Field Quality Studies of SNS Ring Extraction Lambertson Septum Magnet extraction, septum, target, quadrupole 205
 
  • J. G. Wang
    ORNL, Oak Ridge, Tennessee
 
 

Funding: ORNL/SNS is managed by UT-Battelle, LLC, for the U.S. Department of Energy under contract DE-AC05-00OR22725.


3D computer simulations are performed to study magnetic field qualities in the SNS ring extraction Lambertson septum magnet. This work is motivated by the existence of a significant skew quad term in the magnet that has been identified as the source of causing a beam profile distortion on the target. The skew quad term is computed with different methods in simulations and is compared to measurement data. The origin of the large skew quad term is thoroughly investigated. The remedy for minimizing the skew quad term by modifying the magnet is also proposed. Particle tracking has been performed to verify the beam profile evolution through the existing and modified septum. The magnetic interference to the septum performance from an adjacent quadrupole is also assessed. This paper reports our simulation techniques and major results.

 
MO6PFP037 Fabrication and Measurement of 12 GeV Prototype Quadrupoles at Thomas Jefferson National Accelerator Facility quadrupole, magnet-design, controls, multipole 223
 
  • T. Hiatt, K.S. Baggett, J.M. Beck, J.G. Dail, L. Harwood, J. Meyers, M. Wiseman
    JLAB, Newport News, Virginia
 
 

Jefferson Lab’s Continuous Electron Beam Accelerator Facility (CEBAF) currently has maximum beam energy of 6 GeV. The 12 GeV Upgrade Project will double the existing energy and is currently scheduled for completion in 2014. This doubling of energy requires modifications to the beam transport system which includes the addition of several new magnet designs and modifications to many existing designs. Prototyping efforts have been concluded for two different designs of quadrupole magnets required for the upgrade. The design, fabrication and measurement will be discussed.


Authored by Jefferson Science Associates, LLC under U.S. DOE Contract No. DE-AC05-06OR23177.

 
MO6PFP050 Hysteresis Effects of MCBX Magnets on the LHC Operation in Collision injection, controls, collider, superconducting-magnet 250
 
  • N.J. Sammut, C. Giloux, M. Lamont, W. Venturini Delsolaro, S.M. White
    CERN, Geneva
 
 

The Large Hadron Collider beams are brought into collision by superconducting orbit corrector magnets which generate the parallel separation and crossing angles at the interaction points during the different cycle phases. Unfortunately, the magnetic field errors that result from hysteresis effects in the operation region of these magnets lead to unwanted orbit perturbations. In a previous paper, it has been shown that these effects are within the perturbations coming from beam-beam interactions for the MCBC and the MCBY magnets but are significant in the case of the MCBX magnets. This paper presents a refined model of their field in the frame of the Field Description for the LHC (FiDeL), the results obtained from new magnetic measurements in cold conditions to test the model, the powering mechanism employed to maximize their field reproducibility, and the impact the modeling error is predicted to have on the LHC orbit.

 
MO6PFP059 4-Coil Superconducting Helical Solenoid Model for MANX solenoid, quadrupole, dipole, collider 265
 
  • M.J. Lamm, N. Andreev, V. Kashikhin, V.S. Kashikhin, A.V. Makarov, M.A. Tartaglia, K. Yonehara, M. Yu, A.V. Zlobin
    Fermilab, Batavia
  • R.P. Johnson, S.A. Kahn
    Muons, Inc, Batavia
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-06ER86282


Magnets for the proposed muon cooling demonstration experiment MANX (Muon collider And Neutrino factory eXperiment) have to generate longitudinal solenoid and transverse helical dipole and helical quadrupole fields. This paper discusses the 0.4 M diameter 4-coil Helical Solenoid (HS) model design, manufacturing, and testing that has been done to verify the design concept, fabrication technology, and the magnet system performance. The model quench performance in the FNAL Vertical Magnet Test Facility (VMTF) will be discussed.

 
MO6PFP067 Magnetic Field Measurements of HD2, a High Field Nb3Sn Dipole Magnet dipole, sextupole, multipole, quadrupole 283
 
  • X. Wang, S. Caspi, D.W. Cheng, H. Felice, P. Ferracin, R.R. Hafalia, J.M. Joseph, A.F. Lietzke, J. Lizarazo, A.D. McInturff, G.L. Sabbi
    LBNL, Berkeley, California
  • K. Sasaki
    KEK, Ibaraki
 
 

Funding: U.S. Department of Energy


The Superconducting Magnet Program at Lawrence Berkeley National Laboratory has designed and tested HD2, a 1 m long Nb3Sn accelerator-type dipole with a 42 mm clear bore. HD2 is based on a simple block-type coil geometry with flared ends, and represents a step towards the development of cost-effective accelerator quality magnets operating in the range of 13-15 T. The design was optimized to minimize geometric harmonics and to address iron saturation and conductor magnetization effects. Field quality was measured during recent cold tests. The measured harmonics are presented and compared to the design values.

 
MO6PFP077 Magnetic Simulation of a Superconducting Undulator for the Advanced Photon Source undulator, photon, storage-ring, status 310
 
  • Y. Ivanyushenkov
    ANL, Argonne
 
 

Funding: Work supported by U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


A superconducting planar undulator is under development at the Advanced Photon Source (APS). The initial R&D phase of the project includes intensive magnetic modeling performed with the Opera 2d and 3d software packages. This simulation addresses questions of magnetic design of the undulator including calculation of peak field on the undulator axis and maximum field in the conductor, superconductor load line optimization, and design of the undulator ends and correction coils. Results of the magnetic simulation are presented in the paper.

 
MO6PFP085 Simulation of NdFeB Permanent Magnets at Low Temperature permanent-magnet, undulator, cryogenics, insertion-device 327
 
  • G. Lebec, J. Chavanne
    ESRF, Grenoble
  • C. Benabderrahmane
    SOLEIL, Gif-sur-Yvette
 
 

Cryogenic Permanent Magnet Undulators (CPMU) are currently being developed in some Synchrotron Light Sources. Low Temperature NdFeB Permanent Magnets are used to achieve both a high remanence and a high coercive field. Low temperature magnetization hysteresis curves cannot be obtained by a simple transformation of ambient temperature curves; this requires a specific simulation tool. A Monte-Carlo based Permanent Magnet Simulator has been developed at the ESRF. In this simulator, the magnets can be described as a set of several magnetic grains. The model inputs are physical parameters such as anisotropy constants, easy-axis distribution and coercive field. The orientation of magnetic moments are calculated for each grain according to an analytical model and optimization methods are used for fast computations. Magnetization versus external field curves is calculated in a few seconds. This fits with low temperature NdFeB magnetization measurements. These curves have been efficiently used to obtain Radia material parameters for CPMU design.

 
MO6PFP089 Test of a Short Prototype of a Superconducting Undulator for the ANKA Synchrotron Light Source undulator, synchrotron, superconductivity, radiation 339
 
  • E.M. Mashkina, A.J. Magerl
    University Erlangen-Nurnberg, Institute of Condensed Matter Physics, Erlangen
  • C. Boffo, M. Borlein, W. Walter
    BNG, Würzburg
  • S. Casalbuoni, A.W. Grau, M. Hagelstein, D. Saez de Jauregui
    FZK, Karlsruhe
  • N. Vassiljev
    University Erlangen-Nuernberg, Institute of Condensed Matter Physics, Erlangen
 
 

A new 15 mm period, 1.5 m long planar undulator is being fabricated by Babcock Noell GmbH (BNG) for the ANKA synchrotron light source. In order to qualify the production process and to optimize both the quench protection scheme and the magnetic field correction system, a short prototype has been fabricated. The prototype has been tested in vertical configuration and liquid helium at 4.2K in the CASPER facility at ANKA. The magnetic field has been measured along the beam axis direction by Hall probes with a positioning precision of 3 μm. We report here on the field shimming scheme and the resulting performance of the coils.

 
MO6RFP031 A New Approach to the Modelling of the Plasma Dynamics in ECR Ion Sources electron, plasma, ion, ECR 420
 
  • D. Mascali, L. Celona, G. Ciavola, S. Gammino, F. Maimone
    INFN/LNS, Catania
 
 

The trend of ECRIS to higher frequencies and magnetic fields is driven by the need to have higher beam currents and higher charge states for nuclear physics accelerators. Anyway, because of the limits imposed by the magnets’ and microwaves generator’s technology, any further increase of performances requires a detailed investigation of the plasma dynamics. The experiments have shown that the current, the charge states and even the beam shape change by slightly varying the microwave frequency (frequency tuning effect - FTE). Moreover, for last generation ECRIS, electron energies up to 2 MeV have been detected, depending mainly on the magnetic field structure and gradient distribution over the ECR surface. The plasma dynamics have been studied by means of single particle and PIC simulations: they explain the FTE in terms of the wave field distribution over the ECR surface and the existence of high energy electrons due to diffusion in the velocity space above the stochastic barrier. Other methods used to improve the ECRIS performances, e.g. the two frequency heating with an adequate phase relation between the two waves, can be exploited by means of the simulations.

 
MO6RFP034 The EBIT Charge State Booster for Exotic Beam Reacceleration at MSU electron, gun, ion, cathode 429
 
  • O.K. Kester, G. Bollen, M.J. Johnson, M. A. Kostin, J. Ottarson, M. Portillo, S. Schwarz, C. Wilson
    NSCL, East Lansing, Michigan
 
 

The National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University (MSU) is implementing a system to reaccelerate rare isotope beams from projectile fragmentation to energies of about 3 MeV/u. The reacceleration of stopped radioactive beams from projectile fragmentation at the NSCL/MSU makes use of charge state breeding in an Electron Beam Ion Trap (EBIT) to provide a compact and cost efficient system layout of MSU’s ReA3. The MSU EBIT breeder device will provide a high electron beam current density of about 104 A/cm2 making it well suited to rapidly increase the charge state of short-lived isotopes within tens of milliseconds or less. In addition, the breeder is optimized to provide a high storage capacity, a high beam acceptance and uses a continuous injection and beam accumulation scheme explicitly, which makes it unique. To match the beam of singly charged rare isotope ions into the acceptance of the EBIT and to analyze and purify the EBIT beams, a sophisticated beam line and diagnostic system is required. The present paper will present an overview and the status of the ReA3 EBIT.

 
MO6RFP039 Calculation of Charge-Changing Cross Sections of Ions or Atoms Colliding with Fast Ions Using the Classical Trajectory Method ion, electron, target, heavy-ion 442
 
  • I. Kaganovich, R.C. Davidson
    PPPL, Princeton, New Jersey
  • H.E. Mebane
    HCL, Cambridge, Massachusetts
  • A. Shnidman
    PU, Princeton, New Jersey
 
 

Funding: Research supported by the U.S. Department of Energy.


The evaluation of ion-atom charge-changing cross sections is needed for many accelerator applications. A classical trajectory Monte Carlo (CTMC) simulation has been used to calculate ionization and charge exchange cross sections. For benchmarking purposes, an extensive study has been performed for the simple case of hydrogen and helium targets in collisions with various ions. Despite the fact that the simulations only account for classical mechanics effects, the calculated values are comparable to the experimental results for projectile velocities in the region corresponding to the maximum cross section. Shortcomings of the CTMC method for multi-electron target atoms are also discussed.

 
MO6RFP044 An Optimization of a DC Injector with Merger for the Energy Recovery Linac Upgrade to the APS emittance, gun, laser, cavity 455
 
  • X.W. Dong, M. Borland
    ANL, Argonne
 
 

Funding: Work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


An energy recovery linac (ERL) is a potential candidate for an Advanced Photon Source (APS) upgrade at Argonne National Laboratory. A high-DC-voltage photocathode-gun-based electron injector* was previously investigated to meet the ultra-low emittance requirement. Recently the modeling was extended to include a merger using the fully three-dimensional tracking simulation code IMPACT-T. A multiobjective numerical optimization was performed with the goal of delivering a 10-MeV, 19-pC bunch with a normalized transverse emittance less than 0.1 μm at the entrance of the linac. In this paper we show the optimum performance obtained.


*Y.-E. Sun et al., ”Optimization of a DC Injector for an Energy Recovery Linac Upgrade to the Advanced Photon Source”, Proc. of LINAC 2008, TUP100, to be published on http://www.jacow.org.

 
MO6RFP047 High Frequency Bunch Train Generation from an RF Photoinjector at the AWA laser, electron, polarization, wakefield 464
 
  • J.G. Power
    ANL, Argonne
  • C.-J. Jing
    Euclid TechLabs, LLC, Solon, Ohio
  • I. Jovanovic
    Purdue University, West Lafayette, Indiana
 
 

Funding: This work is supported by the U.S. Department of Energy under Contract No. DE-AC02-06CH11357 with Argonne National Laboratory.


An exploratory study for the generation of high frequency bunch trains is underway at the Argonne Wakefield Accelerator (AWA) facility. High frequency bunch trains have numerous applications ranging from advanced acceleration methods to THz radiation sources. Recent studies have shown that such trains can be generated when an intensity modulated laser pulse is incident on the photocathode in the gun. Using the recently developed technique of temporal pulse stacking with UV birefringent crystals* the modulation wavelength obtainable is primarily limited by the UV pulse length. For the AWA photoinjector laser system this limit is about 200 um (rms=670 fs); although using commercially available laser systems this can be as short as 10 um. We present measurements of the intensity modulated laser pulse created with an alpha-BBO crystal array, TStep simulations of the electron beam dynamics, and experimental plans to measure the bunch train using an L-band deflecting mode cavity.


*J.G. Power et al., in Proc. 2008 Advanced Accelerator Concepts, Santa Cruz, Ca., AIP Press, editors C. Schroeder and K. Girardi

 
MO6RFP048 Simulation Study of a Normal-Conducting RF Photoinjector for ERL X-Ray Sources gun, cavity, cathode, emittance 467
 
  • C.-X. Wang
    ANL, Argonne
 
 

Funding: This work was supported by U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


Low-frequency normal-conducting photoinjectors have the potential to generate CW beam due to low frequency and relatively low field. They can provide a much higher accelerating field at the cathode than envisioned DC injectors but without the complexity involved in superconducting rf injectors. Low frequency allows a relatively long bunch near the cathode to reduce space-charge effects, which is detrimental for generating demandingly high-brightness beams. However, low frequency means higher bunch charge for a given average current, counteracting the potential benefits of low-frequency rf injectors. Furthermore, significant bunch length reduction in the injectors is often needed, which may degrade transverse brightness. To explore the potential of a normal-conducting injector for the envisioned ERL upgrade of the Advanced Photon Source, we made a preliminary design and searched for a suitable solution using genetic optimization. Simulation results are presented.

 
MO6RFP053 A Continuous Wave, Normal Conducting, L-Band PWT Photoelectron Gun cavity, gun, vacuum, cathode 479
 
  • D. Yu, Y. Luo
    DULY Research Inc., Rancho Palos Verdes, California
 
 

A Gallium Arsenide (GaAs) photocathode RF electron gun is useful if high polarization (>85%) and low emittance are required as, for example, in the Continuous Electron Beam Accelerator Facility (CEBAF) at the Thomas Jefferson National Accelerator Facility. DULY Research is developing a normal-conducting, L-band photoelectron gun in an ultra high vacuum accelerating structure called the Plane-Wave-Transformer (PWT) integrated with an activated, strained-lattice GaAs photocathode, as a continuous wave polarized electron source. We compare two designs (1-cell and ½ cell) of an L-Band PWT photoelectron gun in this paper. This RF gun will simplify the CEBAF photoinjector design by replacing the direct current (DC) gun, buncher cavities and the capture section. The new compact design provides a stiffer beam that is less subject to space charge blowup. In addition, a higher field gradient at the photocathode would mitigate electron and ion backbombardment problems. Cooling for a CW PWT gun is challenging but manageable.

 
MO6RFP059 Design of a Normal Conducting L-Band Photoinjector cavity, gun, emittance, cathode 497
 
  • J.H. Han
    Diamond, Oxfordshire
 
 

For the successful operation of an X-ray free electron laser the injector must be robust and able to provide a high quality beam. In this paper we present the design of a normal conducting L-band photoinjector which is based on the successful DESY/PITZ gun, but with improved cavity geometry. The result of beam dynamics simulations predicts that a beam with a normalized transverse emittance of less than 0.7 mm mrad at 1 nC can be produced. With an expected repetition rate of at least 1 kHz this gun meets the requirements of the first stage injector for the UK's New Light Source project.

 
MO6RFP060 Numerical Study of the RF Heating of an L-Band Gun cavity, gun, cathode, electron 500
 
  • J.H. Han, H.C. Huang
    Diamond, Oxfordshire
 
 

To precisely control the electron beam parameters from a photocathode RF gun, the RF field distribution during real RF operation must be known. During RF operation, the RF field induces local RF heating on the cavity surface. This non-uniform temperature distribution may deform the cavity and affect the output beam parameters. Here, we model a copper RF gun cavity and calculate the temperature distribution and the stress over the cavity surface. Then, the beam parameter change caused by the cavity deformation is simulated.

 
MO6RFP061 Positron Source Target Survivability Studies target, undulator, radiation, positron 503
 
  • S. Hesselbach, G.A. Moortgat-Pick
    Durham University, Durham
  • I.R. Bailey, L.J. Jenner
    Cockcroft Institute, Warrington, Cheshire
  • J.-L. Fernandez-Hernando
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • S. Riemann, A. Schälicke, A. Ushakov
    DESY Zeuthen, Zeuthen
  • J. Rochford
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • L. Zang
    The University of Liverpool, Liverpool
 
 

Energy deposition in the conversion targets of positron sources for future linear colliders will lead to thermal shock waves which could limit the targets' lifetimes. For the International Linear Collider baseline source, we have studied the energy deposition in a target taking the higher harmonics of the undulator radiation fully into account and applying hydrodynamical models for the resulting heat flow to determine the thermal stress in the target and to assess its survivability.

 
MO6RFP067 Beam Dynamics Simulation for the Compact ERL Injector emittance, space-charge, cavity, cathode 521
 
  • T. Miyajima, Y. Honda, Y. Kobayashi, T.M. Mitsuhashi, T. Muto, S. Sakanaka, M. Shimada
    KEK, Ibaraki
  • R. Hajima
    JAEA/ERL, Ibaraki
 
 

The compact ERL, cERL, is a project to test an energy recovery linac (ERL) with 60 MeV and 100 mA electron beam to generate synchrotron radiation with smaller emittance and shorter pulse length. The design work of the cERL injector has been carried out using a space charge simulation code. The injector consists of 500 kV photo cathode DC gun, two solenoid magnets, buncher cavity, three super conducting RF cavities and merger section to return pass. It generates an electron beam with -77 pC bunch charge and 1.3 GHz repetition rate. Our target value of emittance is less than 1 mm mrad with the bunch length of 1 mm at the exit of the injector. The parameter optimization of the injector using the multi objected method has been carried out to obtain the minimum emittance. The simulation results will be presented in detail.

 
MO6RFP070 Optical Injector Based on Particle Acceleration by Stimulated Emission of Radiation in a Penning-Trap electron, space-charge, radiation, photon 530
 
  • L. Schächter
    Technion, Haifa
 
 

Funding: This work was supported by the Israel Science Foundation and the Kidron Foundation


We present results of an analysis demonstrating that electrons oscillating in a Penning trap may drain the energy stored in an adjacent active medium. For this process to happen, the electrons must become bunched and the energy imparted to the electrons allows them to leave the trap resulting into a train of bunches. Their angular frequency corresponds to medium’s resonance.

 
MO6RFP071 Velocity Bunching Experiments at SPARC emittance, bunching, solenoid, linac 533
 
  • M. Ferrario, D. Alesini, M. Bellaveglia, R. Boni, M. Boscolo, M. Castellano, E. Chiadroni, L. Cultrera, G. Di Pirro, L. Ficcadenti, D. Filippetto, V. Fusco, A. Gallo, G. Gatti, C. Marrelli, M. Migliorati, A. Mostacci, E. Pace, L. Palumbo, B. Spataro, C. Vaccarezza, C. Vicario
    INFN/LNF, Frascati (Roma)
  • G. Andonian, G. Marcus, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • A. Bacci, V. Petrillo, A.R. Rossi, L. Serafini
    Istituto Nazionale di Fisica Nucleare, Milano
  • A. Cianchi, B. Marchetti
    INFN-Roma II, Roma
  • L. Giannessi, M. Labat, M. Quattromini, C. Ronsivalle
    ENEA C.R. Frascati, Frascati (Roma)
  • M. Rezvani Jalal
    University of Tehran, Tehran
  • M. Serluca
    INFN-Roma, Roma
 
 

One of the main goals of the SPARC high brightness photoinjector is the experimental demonstration of the emittance compensation process while compressing the beam with the velocity bunching technique, also named RF compressor. For this reason, the first two S-band travelling wave accelerating structures downstream of the RF gun are embedded in a long solenoid, in order to control the space charge induced emittace oscillations during the compression process. An RF deflecting cavity placed at the exit of the third accelerating structure allows bunch length measurements with a resolution of 50 μm. During the current SPARC run a parametric experimental study of the velocity bunching technique has been performed. The beam bunch length and projected emittance have been measured at 120 MeV as a function of the injection phase in the first linac, and for different solenoid field values. In this paper we describe the experimental layout and the results obtained thus far. Comparisons with simulations are also reported.

 
MO6RFP080 Intense Stopping Muon Beams dipole, target, proton, solenoid 560
 
  • C. Y. Yoshikawa, R.J. Abrams, C.M. Ankenbrandt, M.A.C. Cummings, R.P. Johnson
    Muons, Inc, Batavia
  • M.A. Martens, D.V. Neuffer, M. Popovic, E. Prebys, K. Yonehara
    Fermilab, Batavia
 
 

The study of rare processes using a beam of muons that stop in a target provides access to new physics at and beyond the reach of energy frontier colliders. The flux of stopping muons is limited by the pion production process and by stochastic processes in the material used to slow down the decay muons. Innovative muon beam collection and cooling techniques are applied to the design of stopping muon beams in order to provide better beams for such experiments. Such intense stopping beams will also support the development of applications such as muon spin resonance and muon-catalyzed fusion.

 
MO6RFP085 Study of Transverse Emittance Evolution in 3.5-Cell DC-SC Photo-Injector emittance, FEL, superconducting-cavity, cavity 568
 
  • W. Xu, S.W. Quan, K. Zhao, J. Zhuang
    PKU/IHIP, Beijing
 
 

High quality electron beam with low transverse emittance in 3.5‐cell DC‐SC photo‐injector is crucial significance for PKU‐ERL‐FEL facility. In this paper, we analyse the emittance evolution in the 3.5‐cell DC‐SC photo‐injector by simply model with consideration of DC acceleration, RF acceleration and space charge effect. The results are compared with Astra simulation. The matching condition of DC‐gun and Superconducting cavity, which is critical for the final emittance at the exit of the injector, is also presented.

 
MO6RFP087 Thermionic Cathode-Grid Assembly Simulations for RF Guns emittance, cathode, gun, cavity 572
 
  • V. Volkov, E. Kenzhbulatov, S.A. Krutikhin, G.Y. Kurkin, V.M. Petrov, E. Rotov, N. Vinokurov
    BINP SB RAS, Novosibirsk
 
 

The projected electron RF gun of Novosibirsk Microtron-Recuperator injector employs an industrial thermionic cathode grid assembly with 0.08 mm gap that usually used in metal-ceramic RF tubes. Three-dimensional (3D)computer simulations have been performed that use the mesh refinement capability of the both Microwave Studio and 2D SAM codes to examine the full region of the real cathode grid assembly in static fields in order to illustrate the beam quality that can result from such a gridded structure. These simulations have been found to reproduce the beam current behaviors versus of applied potentials that are observed experimentally. Based on it ASTRA RF beam simulations also predict a complicated time-dependent response to the waveform applied to the grid during the current turn-on, calculation of the dissipated power by electrons at the grid, and particle tracking downstream of the grid into RF gun cavity and farther on. These simulations may be representative in other sources, such as some L-band RF injectors for industrial applications.

 
MO6RFP091 A Laser-Cooled Electron Source for Ultrafast Electron Diffraction electron, laser, cathode, brightness 580
 
  • S.B. van der Geer, B. Fleskens, O.J. Luiten, M.P. Reijnders, G. Taban, E.J.D. Vredenbregt
    TUE, Eindhoven
  • S.B. van der Geer
    Pulsar Physics, Eindhoven
 
 

Ultrafast electron diffraction (UED) enables single-shot studies of structural dynamics at atomic length and time scales, i.e. 0.1 nm and 0.1 ps. At present UED experiments are based on femtosecond laser photoemission from solid state cathodes. We propose a new type of electron source, based on near-threshold photoionization of a laser-cooled and trapped atomic gas. The electron temperature of these sources can be as low as 10 K. This implies an increase in brightness by orders of magnitude and enables single-shot studies of, e.g., biomolecular samples. In this contribution we numerically investigate the performance of a laser-cooled electron source by GPT tracking simulations with realistic fields and all pairwise Coulomb interactions.

 
MO6RFP095 The Megaelectron-Volt Ultrafast Electron Diffraction Experiment at Tsinghua University electron, laser, gun, cavity 590
 
  • R.K. Li, H. Chen, Q. Du, T. Du, Y.-C. Du, W.-H. Huang, J. Shi, C.-X. Tang, L.X. Yan
    TUB, Beijing
  • X.J. Wang
    BNL, Upton, Long Island, New York
 
 

Funding: Supported by National Natural Science Foundation of China (No.10735050, No.10875070) and National Basic Research Program of China (973 Program)(No.2007CB815102)


Time-resolved MeV ultra-fast electron diffraction (UED) is a promising tool for studying of structural dynamics on the fundamental temporal and spatial scales of atomic motion. To reach the desired temporal and spatial resolutions, precise control and measurement of ultra-short, low emittance electron pulses are required. A MeV UED system based on an S-band photocathode RF gun is built and optimized at Tsinghua University. We present the experiment results here.

 
MO6RFP096 Beam Slice Characterization at SPARC High Brightness Photoinjector emittance, FEL, quadrupole, bunching 593
 
  • A. Cianchi
    Università di Roma II Tor Vergata, Roma
  • D. Alesini, M. Bellaveglia, M. Castellano, E. Chiadroni, L. Cultrera, G. Di Pirro, M. Ferrario, D. Filippetto, G. Gatti, E. Pace, C. Vaccarezza, C. Vicario
    INFN/LNF, Frascati (Roma)
  • L. Ficcadenti, A. Mostacci
    Rome University La Sapienza, Roma
  • B. Marchetti
    INFN-Roma II, Roma
  • C. Ronsivalle
    ENEA C.R. Frascati, Frascati (Roma)
 
 

The SPARC photoinjector drives a SASE FEL to perform several experiments both for the production of high brightness electron beam and for testing new scheme of SASE radiation generation. The control of the beam properties, in particular at the level of the slice dimension, is crucial in order to optimize the FEL process. We report the different measurements performed in order to characterize the slice properties of the electron beam.

 
MO6RFP099 A Single Bunch Electron Gun for the ANKA Injector gun, emittance, cathode, electron 602
 
  • A. Hofmann, M. Fitterer, M. Klein, A.-S. Müller, K.G. Sonnad
    KIT, Karlsruhe
  • G. Blokesch
    PPT, Dortmund
  • E. Huttel, N.J. Smale
    FZK, Karlsruhe
  • S. Marsching, T. Weis
    DELTA, Dortmund
  • C. Piel
    ACCEL, Bergisch Gladbach
  • R. Weigel
    Max-Planck Institute for Metal Research, Stuttgart
 
 

Funding: This work has been supported by the Initiative and Networking Fund of the Helmholtz Association under contract number VH-NG-320.


The microtron of the ANKA injector is presently equipped with a diode- type electron gun, which produces long pulses. A new thermionic DC triode-type electron gun has been ordered and foreseen for installation in the ANKA injector. The new gun allows single bunch as well as long pulse operation, thus offering the possibility to study beam properties in single bunch operation. This is particularly of interest for the investigation of the short bunch dynamics in the generation of coherent THz radiation. Furthermore, the new gun will make time resolved measurement possible. Simulations of the gun-to-microtron transport with special emphasis on the emittance evolution e.g. due to space charge have been done. Measurements of the gun performance are presently underway and are summarised in this paper.

 
TU1PBI01 Fully 3D Multiple Beam Dynamics Processes Simulation for the Tevatron proton, beam-beam-effects, dipole, emittance 630
 
  • E.G. Stern, J.F. Amundson, P. Spentzouris, A. Valishev
    Fermilab, Batavia
 
 

Extensive work has been done to create an accurate model of beam dynamics at the Fermilab Tevatron. This talk will present validation and results from the development of a simulation of the machine including multiple beam dynamics effects. The essential features of the simulation include a fully 3D strong-strong beam-beam particle-in-cell Poisson solver, interactions among multiple bunches and both head-on and long-range beam-beam collisions, coupled linear optics and helical trajectory consistent with beam orbit measurements, chromaticity and resistive wall impedance. The individual physical processes are validated against measured data where possible, and analytic calculations elsewhere. The simulation result discussion will focus on the effects of increasing beam intensity with single and multiple bunches on the impedance of the beams.

 

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TU1PBI02 Simulating Electron-Ion Dynamics in Relativistic Electron Coolers electron, ion, luminosity, FEL 635
 
  • D.L. Bruhwiler
    Tech-X, Boulder, Colorado
 
 

Funding: Supported by the US DOE Office of Science, Office of Nuclear Physics under grants DE-FC02-07ER41499 and DE-FG02-08ER85182; used NERSC resources under grant DE-AC02-05CH11231.


Novel electron-ion collider (EIC) concepts are a high priority for the long-term plans of the international nuclear physics community. Orders of magnitude higher luminosity will be required for the relativistic ion beams in such accelerators. Electron cooling is a promising approach to achieve the necessary luminosity. The coherent electron cooling (CEC) concept proposes to combine the best features of electron cooling and stochastic cooling, via free-electron laser technology, to cool high-energy hadron beams on orders-of-magnitude shorter time scales*. In a standard electron cooler, the key physical process is dynamical friction on the ions. The modulator section of a coherent cooler would be very similar to a standard cooler, but in this case dynamical friction becomes irrelevant and the key physics is the shape of the density wake imprinted on the electron distribution by each ion. We will present results using the massively parallel VORPAL framework for both particle-in-cell (PIC) and molecular dynamics (MD) simulations of electron-ion collisions in relativistic coolers and CEC modulators.


* V.N. Litvinenko, I. Ben-Zvi, M. Blaskiewicz, Y. Hao, D. Kayran, E. Pozdeyev, G. Wang, G.I. Bell, D.L. Bruhwiler, A.V. Sobol et al., FEL Conf. Proc. (2008), in press.

 

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TU1PBI04 Application of the Reduction of Scale Range in a Lorentz Boosted Frame to the Numerical Simulation of Particle Acceleration Devices laser, electron, plasma, injection 641
 
  • J.-L. Vay, E. Cormier-Michel, W.M. Fawley, C.G.R. Geddes
    LBNL, Berkeley, California
  • D.P. Grote
    LLNL, Livermore, California
 
 

Funding: Supported by the US DOE at LBNL and LLNL under contracts DE-AC02-05CH11231 and DE-AC52-07NA27344, LARP, SciDAC, and ComPASS. Computuational resources of the NERSC were employed.


It has been shown* that the ratio of longest to shortest space and time scales of a system of two or more components crossing at relativistic velocities is not invariant under Lorentz transformation. This implies the existence of a frame of reference minimizing an aggregate measure of the ratio of space and time scales. It was demonstrated that this translated into a reduction by orders of magnitude in computer simulation run times, using methods based on first principles (e.g., Particle-In-Cell), for particle acceleration devices and for problems such as: free electron laser, laser-plasma accelerator, and particle beams interacting with electron clouds. Since then, speed-ups ranging from 75 to more than four orders of magnitude have been reported for the simulation of either scaled or reduced models of the above-cited problems. In ** it was shown that to achieve full benefits of the calculation in a boosted frame, some of the standard numerical techniques needed to be revised. The theory behind the speed-up of numerical simulation in a boosted frame, latest developments of numerical methods, and example applications with new opportunities that they offer are all presented.


* J.-L. Vay, Phys. Rev. Lett. 98, 130405 (2007).
**J.-L. Vay, Phys. of Plasmas 14, 1 (2008).

 

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TU2RAI01 Development of the IFMIF/EVEDA Accelerator rfq, linac, cavity, emittance 663
 
  • A. Mosnier
    CEA, Gif-sur-Yvette
 
 

With the aim of producing an intense flux of 14 MeV neutrons, the International Fusion Materials Irradiation Facility (IFMIF) relies on two high power CW accelerator drivers, each delivering a 125 mA deuteron beam at 40 MeV to a common lithium target. The Engineering Validation and Engineering Design Activities (EVEDA) phase of IFMIF, which has been launched in the middle of 2007, has two major objectives: to produce the detailed design of the entire IFMIF facility and to build and test the key systems, in particular the prototype of a high-intensity CW deuteron accelerator (125 mA @ 9 MeV). The design of the IFMIF accelerator, as well as the design of the prototype to be installed in Rokkasho (Japan) are presented.

 

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TU2PBC01 Space-Charge Simulations of Non-Scaling FFAGs Using PTC space-charge, resonance, acceleration 673
 
  • D.T. Abell, G.I. Bell, A.V. Sobol
    Tech-X, Boulder, Colorado
  • E. Forest
    KEK, Ibaraki
  • A.G. Ruggiero, D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

Funding: Supported in part by the DOE Office of Science, Office of Nuclear Physics under grant No. DE-FG02-06ER84508.


Non-scaling FFAGs are sensitive to a slew of resonances during the acceleration ramp. An important consideration - because it affects the amount of rf power required - will be the speed at which resonances must be crossed. We present simulations of possible non-scaling FFAGs, focusing especially on the effects of space charge, using newly developed capabilities in the code PTC*.


* E. Forest, Y. Nogiwa, F. Schmidt, "The FPP and PTC Libraries", ICAP'2006.

 

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TU2PBC04 Transport of Ultra-Short Electron Bunches in a Free-Electron Laser Driven by a Laser-Plasma Wakefield Accelerator quadrupole, electron, undulator, FEL 680
 
  • M.P. Anania, D. Clark, R.C. Issac, D.A. Jaroszynski, A. J. W. Reitsma, G.H. Welsh, S.M. Wiggins
    USTRAT/SUPA, Glasgow
  • J.A. Clarke, M.W. Poole, B.J.A. Shepherd
    Cockcroft Institute, Warrington, Cheshire
  • M.J. de Loos, S.B. van der Geer
    Pulsar Physics, Eindhoven
 
 

Funding: The U.K. EPSRC and the European Community - New and Emerging Science and Technology Activity under the FP6 “Structuring the European Research Area” programme (project EuroLEAP, contract number 028514)


The Advanced Laser-Plasma High-Energy Accelerators towards X-rays (ALPHA-X) programme* is developing laser-plasma accelerators for the production of ultra-short electron bunches as drivers of incoherent and coherent radiation sources from plasma and magnetic undulators. Focusing of ultra-short electron bunches from a laser-plasma wakefield accelerator into an undulator requires that particular attention be paid to the electron beam quality. We will discuss the design and implementation of an upgraded focusing system for the ALPHA-X beam line, which currently consists of a triplet of electromagnet quadrupoles. The upgrade will comprise the installation of additional compact permanent quadrupoles** very close to the accelerator exit. This will improve the matching of the beam into the undulator. The design has been carried out using the General Particle Tracer (GPT) code*** and TRANSPORT code, which consider space charge effects and allow a realistic estimate of electron beam properties inside the undulator to be obtained. We will present a study of the influence of beam transport on free-electron laser action in the undulator, paying particular attention to bunch dispersion.


* D. Jaroszynski et al., Phil. Trans. R. Soc. A 364, 689-710 (2006)
** T. Eichner et al., Phys. Rev. ST Accel. Beams 10, 082401 (2007)
*** S.B. Geer, M.J. Loos, Ph.D. thesis, TU/e, Eindhoven (2001)

 

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TU3PBI02 Linac Code Benchmarking with High Intensity Experiments at the UNILAC DTL, emittance, resonance, space-charge 719
 
  • L. Groening, W.A. Barth, W.B. Bayer, G. Clemente, L.A. Dahl, P. Forck, P. Gerhard, I. Hofmann, M. Kaiser, M.T. Maier, S. Mickat, T. Milosic, G.A. Riehl, H. Vormann, S.G. Yaramyshev
    GSI, Darmstadt
  • D. Jeon
    ORNL, Oak Ridge, Tennessee
  • R. Tiede
    IAP, Frankfurt am Main
  • D. Uriot
    CEA, Gif-sur-Yvette
 
 

Funding: We acknowledge the support of the European Community-Research Infrastructure Activity under the FP6 ‘‘Structuring the European Research Area’’ program (CARE, Contract No. RII3-CT-2003-506395).


Beam dynamics experiments with high intensity beams have been conducted at the GSI UNILAC in 2006-2008 with the goal of benchmarking four major simulation codes, i.e. DYNAMION, PARMILA, TraceWin/PARTRAN and LORASR with respect to transverse emittance growth along a DTL. The experiments comprised measurements of transverse phase space distributions in front of as well as behind the DTL. Additional longitudinal bunch length measurements at the DTL entrance allowed for estimate and control of mismatch in all three planes. Measured effects of mismatch and of theoretically predicted space charge resonances (equipartitioning and others) are compared with simulations for a wide range of transverse phase advance along the DTL. This contribution is the first report on the successful measurement of a space charge driven fourth order resonance in a linear accelerator.

 

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TU3PBC03 Transverse Schottky Noise with Space Charge space-charge, synchrotron, betatron, ion 724
 
  • O. Boine-Frankenheim, V. Kornilov, S. Paret
    GSI, Darmstadt
 
 

The effect of space charge on the transverse Schottky spectrum of coasting and bunched beams is studied using measurements and simulations together with analytic models. The measurements of transverse Schottky bands from heavy ion beams are performed in the SIS-18 synchrotron at GSI. In addition we analyze the noise spectrum from a particle tracking code with self-consistent space charge. Both results are compared to analytic models for coasting and for bunched beams with space charge. For coasting beams an analytic model based on the transverse dispersion relation with linear space and chromaticity reproduces the characteristic deformation of Schottky bands with increasing space charge, observed in both measurement and simulation. For bunched beams we find good agreement between the observed shifts of synchrotron satellites and a simplified model for head-tail modes with space charge. The relevance of the results for the analysis of transverse beam stability in the presence of space charge is emphasized.

 

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TU3PBC04 Circularly Inclined Solenoid Channel for 6D Ionization Cooling of Muons solenoid, damping, cavity, emittance 727
 
  • Y. Alexahin
    Fermilab, Batavia
 
 

Funding: Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the United States Department of Energy


Ionization cooling is essential for realization of Muon Collider, muons beam based neutrino factories and other experiments involving muons. The simplest structure - absorber(s) immersed in alternating solenoidal magnetic field - provides only transverse cooling since the longitudinal motion in the most suitable momentum range (2-300MeV/c) is naturally antidamped. To overcome this difficulty it is proposed to periodically tilt solenoids so that a rotating transverse magnetic field was created. By choosing the phase advance per period above a multiple of 2pi it is possible to ensure that muons with higher momentum make a longer path in the absorber (whether distributed or localized) thus providing longitudinal damping. Basic theory of such channel and results of tracking simulations are presented.

 

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TU3PBC05 Space Charge Simulation on High Intensity Cyclotrons: Code Development and Applications space-charge, cyclotron, single-bunch, acceleration 730
 
  • J.J. Yang, Y. Z. Lin
    TUB, Beijing
  • A. Adelmann
    PSI, Villigen
  • S. An, Y.J. Bi, S.M. Wei, J.J. Yang, T.J. Zhang
    CIAE, Beijing
 
 

In high intensity cyclotrons with small turn separation, both the space charge effects of single bunch and the interaction of radially neighbouring bunches play important roles. A PIC-based three-dimensional parallel code, OPAL-CYCL, is newly developed under OPAL framework which self-consistently covers these two collective effects. In this paper we also present the simulation results from the compact cyclotron CYCIAE-100 in the context of the ongoing upgrade program of BRIF at CIAE, with the goal of 100 MeV, 200 μA CW proton beam on target.

 

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TU3PBC06 Recent Development at the NSCL Small Isochronous Ring ion, extraction, space-charge, injection 733
 
  • Y. Li, G. Machicoane, F. Marti, T.P. Wangler
    NSCL, East Lansing, Michigan
  • E. Pozdeyev
    BNL, Upton, Long Island, New York
 
 

Funding: this work is supported by National Science Foundation Grant PHY-0606007.


The Small Isochronous Ring (SIR) at the NSCL/MSU was built to study space charge effects in the isochronous regime. Results of experimental studies of the longitudinal beam dynamics in the ring showed a remarkable agreement with results of numerical simulations. Recently, we have designed and built an energy analyzer to accurately measure the beam energy spread. We will present results of energy spread measurements as well as simulations of the beam behavior based on the Vlasov formalism.

 

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TU4RAI02 Development of a 10 MW Sheet Beam Klystron for the ILC cavity, klystron, gun, cathode 762
 
  • D.W. Sprehn, A.A. Haase, A. Jensen, E.N. Jongewaard, D.W. Martin
    SLAC, Menlo Park, California
  • A.T. Burke
    SAIC, Billerica, Massachusetts
 
 

Funding: Work supported by Department of Energy contract DE-AC02-76SF00515


SLAC is developing a 10 MW, 5 Hz, 1.6 ms, L-band (1.3 GHz) Sheet-Beam Klystron as a less expensive and more compact alternative to the ILC baseline Multiple-Beam Klystron. The Klystron is intended as a plug-compatible device of the same beam current and operating voltage as existing Multiple-Beam Klystrons. At this time, a beam tester has been constructed and currently is in test. The beam tester includes an intercepting cup for making beam quality measurements of the 130 A, 40-to-1 aspect ratio beam. Measurements will be made of the electrostatic beam and of the beam after transporting through a drift tube and magnetic focusing system. General theory of operation, design trade-offs, and manufacturing considerations of both the beam tester and klystron will be discussed.

 

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TU4RAC03 Modeling and Design of High-Power Inductive Output Tubes cavity, electron, gun, cathode 767
 
  • E.L. Wright, K.T. Nguyen
    Beam-Wave Research, Inc., Union City
  • I.A. Chernyavskiy, J.J. Petillo
    SAIC, McLean
  • S.J. Cooke, B. Levush, J.A. Pasour
    NRL, Washington, DC
  • J.F. DeFord, B. Held
    STAAR/AWR Corporation, Mequon
 
 

Funding: Research funded by the Office of Naval Research and Naval Research Laboratory.


The accelerator community is making the transition to IOT technology for a number of high-power UHF and L-band applications as a result their inherent benefits. Scientists, funded by the Office of Naval Research and Naval Research Laboratory, are investigating the physics of the beam-wave interaction of the IOT. The time-domain electrostatic PIC code MICHELLE, in conjunction with the Analyst® suite of electromagnetic codes, were used to model the cathode-grid-anode structure that comprise the input cavity. Our investigation has led to the discovery of a delay mechanism responsible for intra-bunch charge formation, as evidenced by IOT X-ray generation with energies significantly higher than the cathode accelerating potential, increasing with RF output power. Time-domain PIC results of this effect will be shown. We will also present simulation results of the large-signal beam wave interaction in the output cavity using the code TESLA. Examples of single beam and multiple-beam IOTs will also be shown.

 

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TU4PBC04 Production and Testing Results of Superconducting Cavities for ISAC-II High Beta Section cavity, ISAC, multipactoring, TRIUMF 786
 
  • V. Zvyagintsev, T. Bohdanowicz, R.J. Dawson, K. Fong, A. Grassellino, P.R. Harmer, D. Kishi, R.E. Laxdal, M. Marchetto, A.K. Mitra, T.C. Ries, I. Sekachev, B.S. Waraich, D. Yosifov, Q. Zheng
    TRIUMF, Vancouver
  • R. Edinger
    PAVAC, Richmond, B.C.
 
 

The ISAC-II heavy ion linear accelerator has been in operation at TRIUMF since 2006. The high beta section of the accelerator, consisting of twenty cavities with optimum beta=0.11, is currently under production and is scheduled for completion in 2009. The cavities are superconducting bulk Niobium two-gap quarter-wave resonators with a frequency of 141 MHz, providing, as a design goal, a voltage gain of Veff=1.08 MV at 7 W power dissipation. Production of the cavities is with a Canadian company, PAVAC Industries of Richmond, B.C. after two prototype cavities were developed, produced and successfully tested. Cavity production details and test results will be presented and discussed.

 

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TU4GRI03 The MERIT High-Power Target Experiment at the CERN PS proton, target, solenoid, factory 795
 
  • K.T. McDonald
    PU, Princeton, New Jersey
  • J.R.J. Bennett
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • O. Caretta, P. Loveridge
    STFC/RAL, Chilton, Didcot, Oxon
  • A.J. Carroll, V.B. Graves, P.T. Spampinato
    ORNL, Oak Ridge, Tennessee
  • I. Efthymiopoulos, A. Fabich, F. Haug, J. Lettry, M. Palm, H. Pereira
    CERN, Geneva
  • H.G. Kirk, H. Park, T. Tsang
    BNL, Upton, Long Island, New York
  • N.V. Mokhov, S.I. Striganov
    Fermilab, Batavia
 
 

The MERIT (MERcury Intense Target) experiment was run in the fall of 2007 using 14 and 24 GeV intense proton beams from the CERN PS. It is a proof-of-principle experiment designed to validate a target concept for producing an intense muon source for a future muon collider or neutrino factory. The experiment successfully demonstrated a target technique for multi-MW proton beams that utilizes a free-flowing liquid metal jet within the confines of a high-field solenoid. We describe the experimental strategy and parameters, as well as the results obtained and their implications for future muon-based accelerator facilities.

 

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TU5PFP004 Effect of External Magnetic Fields on the Operation of RF Cavities cavity, electron, space-charge, collider 809
 
  • D. Stratakis, J.S. Berg, J.C. Gallardo, R. B. Palmer
    BNL, Upton, Long Island, New York
 
 

Funding: This work supported by the U.S. Department of Energy, contract no. DE-AC02-98CH10886.


Beam cooling for a future neutrino factory or muon collider requires high gradient rf cavities in the presence of strong magnetic fields. Experimental measurements suggested that the maximum accelerating gradient drops as the axial magnetic field increases. Little is known about the explicit dependence of the gradient on the strength of the magnetic field. The experimental observation of dark currents arising from local regions with enhanced surface field intensities under external magnetic fields however, suggests a new possible mechanism of breakdown based on electron field emission. A model of magnetic field breakdown is proposed. We illustrate that the field emitted electrons are focused by the external fields into small spots on the other side of the cavity and estimate the energy density they deliver to the wall. We show that this energy increases with the magnetic field, and this may lead to melting of the cavity surface. The influence of local fields at the emitter side is discussed and the extent to which space-charge affects this process is investigated. Results of our model are compared with recent experimental data from the 201 MHz and 805 MHz cavities.

 
TU5PFP005 Transfer Matrix Method Used in RF Tuning on DTL for CSNS cavity, DTL, focusing, linac 812
 
  • Z.R. Sun, S. Fu, J. Peng
    IHEP Beijing, Beijing
 
 

In the conventional 324 MHz DTL designed for China Spallation Neutron Source (CSNS) accelerating H- ion from 3MeV to 132MeV, there are 7 tanks and currently the R&D of tank-1 is under proceeding, which has 29 cells and 29 quadrupoles. In design, the Tank-1 has a tilt field distributed partially in order to obtain most effective energy gain and low Kilpatric parameter. In order to decrease the difficulty of tuning the partial tilt field distribution, a new analysis named transfer matrix method is introduced. Verifying of the calculation and simulation of the transfer matrix has been finished with MDTFISH code, picking parameters from CSNS and SNS. Checking the method on the model tank in CSNS will be operated.

 
TU5PFP010 Multipactor in Dielectric Loaded Accelerating Structures multipactoring, electron, vacuum, resonance 827
 
  • P. Schoessow, C.-J. Jing, A. Kanareykin
    Euclid TechLabs, LLC, Solon, Ohio
  • W. Gai, J.G. Power
    ANL, Argonne
  • O.V. Sinitsyn
    UMD, College Park, Maryland
 
 

Funding: Work supported by the US Department of Energy.


The development of high gradient rf driven dielectric accelerating structures is in part limited by the problem of multipactor. The first high power experiments with an 11.424-GHz rf driven alumina accelerating structure exhibited single surface multipactor. Unlike the well understood multipactor problem for dielectric rf windows, where the rf electric field is tangential and the rf power flow is normal to the dielectric surface, strong normal and tangential rf electric fields are present from the TM01 accelerating mode in the DLA and the power flow is parallel to the surface at the dielectric-beam channel boundary. While a number of approaches have been developed, no one technology for MP mitigation is able to completely solve the problem. In this paper we report on numerical calculations of the evolution of the MP discharge, and give particular attention to MP dependence on the rf power ramp profile and the use of engineered surface features on the beam channel wall to interrupt the evolution of the multipactor discharge.

 
TU5PFP011 A Novel Technique for Mitigating Multipactor by Means of Magnetic Surface Roughness multipactoring, electron, cavity, vacuum 830
 
  • F. Caspers, E. Montesinos
    CERN, Geneva
  • S. Anza, J. Gil, C. Vicente
    aurorasat, Paterna
  • V.E. Boria
    DCOM-iTEAM-UPV, Valencia
  • W. Bruns
    WBFB, Berlin
  • L. Conde
    Universidad Politecnica de Madrid, ETSI Aeronauticos, Madrid
  • L. Galan
    UAM, Madrid
  • B. Gimeno
    UVEG, Burjasot (Valencia)
  • C. Miquel Espanya, D. Raboso
    ESA-ESTEC, Noordwijk
  • I. Montero
    CSIC, Madrid
 
 

Multipactor phenomena which are closely linked to the SEY (secondary electron yield) can be mitigated by many different methods including groves in the metal surface as well as using electric or magnetic bias fields. However frequently the application of global magnetic or electric bias field is not practicable considering the weight and power limitations on-board satellites. Additionally, surface grooves may degrade the RF performance. Here we present a novel technique which is based on a magnetostatic field pattern on the metallic surface with fast spatial modulation in the order of 30 micron. This field pattern is produced by proper magnetization of an underlying ferromagnetic layer such as nickel. Simulations and preliminary experimental results will be shown and a number of applications, both for particle accelerators and satellite microwave payloads are discussed.

 
TU5PFP012 Statistical Modeling of DC Sparks cathode, site, vacuum, cavity 833
 
  • Y.I. Levinsen, S. Calatroni, A. Descoeudres, M. Taborelli, W. Wuensch
    CERN, Geneva
 
 

The understanding of electrical breakdowns has a critical role in the design of the RF accelerating cavities for the CLIC linear collider. In this context a new statistical model of the conditioning process and breakdown rate evolution is presented for a DC spark system with tip-plane electrode geometry charged from a capacitance. The approach requires a small amount of assumptions, but can still make several interesting predictions. Electrode gap distance dependence on the saturated breakdown field and spitfest (grouped breakdowns) are among the phenomena that could be explained from this simple model.

 
TU5PFP013 Quantitative Outgassing Studies in DC Electrical Breakdown vacuum, cavity, ion, cathode 836
 
  • Y.I. Levinsen, S. Calatroni, A. Descoeudres, M. Taborelli, W. Wuensch
    CERN, Geneva
 
 

Electrical breakdown in the accelerating cavities set a potential limit to the performance of the CLIC linear collider. Vacuum degradation and beam instability are possible outcomes from a breakdown if too much gas is released from the cavity surface. Quantitative data of gas release are provided for copper electrodes (milled Cu-OFE, as-received and heat-treated), and molybdenum electrodes. These data are produced from a controlled DC spark environment with capacitance charged anode at fixed energy.

 
TU5PFP016 Rapidly Tunable RF Cavity for FFAG Accelerators cavity, proton, ion, DTL 843
 
  • D.J. Newsham, N. Barov, J.S. Kim
    Far-Tech, Inc., San Diego, California
 
 

The fixed-field alternate gradient (FFAG) synchrotron offers an attractive solution for systems that require rapid acceleration over a wide range of energies. The ability to rapidly tune the frequency of the accelerating cavity in the “non-scaling” variety of an FFAG synchrotron represents a fundamental barrier to their implementation in a wide variety of applications for proton, ion and muon acceleration. Initial results of the rapidly tunable cavity design for specific application to proton and light ion medical FFAG accelerators are presented.

 
TU5PFP020 Doped H2-Filled RF Cavities for Muon Beam Cooling electron, cavity, proton, pick-up 855
 
  • K. Yonehara, M. Chung, M. Hu, A. Jansson, A. Moretti, M. Popovic
    Fermilab, Batavia
  • M. Alsharo'a, R.P. Johnson, M.L. Neubauer, R. Sah
    Muons, Inc, Batavia
  • D. Rose, C.H. Thoma
    Voss Scientific, Albuquerque, New Mexico
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-08ER86350 and and FRA DOE contract number DE-AC02-07CH11359


RF cavities pressurized with hydrogen gas may provide effective muon beam ionization cooling needed for muon colliders. Recent 805 MHz test cell studies reported below include the first use of SF6 dopant to reduce the effects of the electrons that will be produced by the ionization cooling process in hydrogen or helium. Measurements of maximum gradient in the Paschen region are compared to a simulation model for a 0.01% SF6 doping of hydrogen. The observed good agreement of the model with the measurements is a prerequisite to the investigation of other dopants.

 
TU5PFP021 Traveling Wave RF Systems for Helical Cooling Channels coupling, acceleration, collider, cavity 858
 
  • K. Yonehara, A. Lunin, A. Moretti, M. Popovic, G.V. Romanov
    Fermilab, Batavia
  • R.P. Johnson, M.L. Neubauer
    Muons, Inc, Batavia
  • L. Thorndahl
    CERN, Geneva
 
 

Funding: supported in part by USDOE STTR Grant DE-FG02-08ER86350


The great advantage of the helical ionization cooling channel (HCC) is its compact structure that enables the fast cooling of muon beam 6-dimensional phase space. This compact aspect requires a high average RF gradient, with few places that do not have cavities. Also, the muon beam is diffuse and requires an RF system with large transverse and longitudinal acceptance. A traveling wave system can address these requirements. First, the number of RF power coupling ports can be significantly reduced compared with our previous pillbox concept. Secondly, by adding a nose on the cell iris, the presence of thin metal foils traversed by the muons can possibly be avoided. We show simulations of the cooling performance of a traveling wave RF system in a HCC, including cavity geometries with inter-cell RF power couplers needed for power propagation.

 
TU5PFP024 Design of an MA Based RF System for the Collector Ring at FAIR cavity, controls, impedance, power-supply 867
 
  • U. Laier, P. Hülsmann, K.-P. Ningel, G. Schreiber
    GSI, Darmstadt
 
 

The 'Facility of Antiproton and Ion Research' (FAIR) project will be realized at the 'GSI Helmholtzzentrum für Schwerionenforschung GmbH' (Darmstadt, Germany) in the scope of a large international collaboration. One of the FAIR storage rings is the collector ring (CR) whose main purpose is to allow a fast cooling of secondary beams (rare isotopes and antiprotons). The RF system of the collector ring has to allow pulsed operation (40kV, duty cycle 5e-4) as well as continuous operation (2kV) in the frequency range of 1.2 to 1.4MHz. The detailed conceptual design of this RF system is introduced here. It will be based (similar to the existing RF system 'SIS18 bunch compressor' which will also be presented at PAC09) on two inductively loaded quarter wavelength coaxial resonators operating on a common ceramic gap. The resonator will be loaded with twelve ring cores (rout=313mm, rin=145mm, h=25mm) of a cobalt based amorphous magnetic alloy (VitroVac6030F); it will be cooled by forced air. The cavity will be driven by a push-pull amplifier operated in class A consisting of two tetrodes (TH555A) that will be coupled inductively to the cavity.

 
TU5PFP025 The New CW RFQ Prototype rfq, linac, impedance, DTL 870
 
  • U. Bartz, A. Bechtold, J.M. Maus, N. Mueller, A. Schempp
    IAP, Frankfurt am Main
 
 

A short RFQ prototype was built for tests of high power RFQ structures. We will study thermal effects and determine critical points of the design. Simulations with CST Microwave Studio and first measurements were done. First results and the status of the project will be presented.

 
TU5PFP036 Design of the Fundamental Mode Damper and the HOM Dampers for the 56 MHz SRF Cavity cavity, HOM, SRF, higher-order-mode 900
 
  • H. Hahn, S. Bellavia, I. Ben-Zvi, E. M. Choi
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


A 56 MHz Superconducting RF cavity is developed for the luminosity enhancement of the Relativistic Heavy Ion Collider (RHIC). The 56 MHz SRF cavity enables to adiabatically rebucket the beam from the 28 MHz accelerating cavities, which with shorter bunch lengths will enhance the luminosity significantly. The 56 MHz SRF cavity fundamental mode must be damped during injection and acceleration by a fundamental mode damper (FD), which is physically withdrawn at store for operation. The cavity frequency changes from the withdrawing motion but is kept below the beam frequency at store by a judicious axial placement of the FD. Physics studies by numerical simulations, tests of the FD in the prototype cavity, and the challenging engineering issues are here addressed. In addition, higher-order mode (HOM) dampers are necessary for the stable operation of the 56 MHz SRF cavity. The HOM’s are identified and the external Q factors are obtained from tests of the prototype cavity and are compared to simulations with the CST MWS program. The HOM damper blocks the fundamental mode by a 5 element high pass filter. The HOM stability criteria of the cavity are satisfied with four HOM dampers.

 
TU5PFP037 Ripple Structure in 56 MHz Quarter Wave Resonator for Multipacting Suppression electron, cavity, niobium, superconductivity 903
 
  • I. Ben-Zvi, D. Naik
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


A beam excited 56 MHz RF Niobium Quarter Wave Resonator has been proposed to enhance RHIC beam luminosity and bunching. As multipacting is expected, an extensive study was carried out with the Multipac 2.1 code, looking for a way to suppress it. Multipacting bands were found. Discharge occurred at cavity’s top corner above beam gap and on outer conductor up to more than half its length, moving towards the end of the cavity. We find single-point multipacting, with emission from the outer conductor, as well as two-point multipacting involving both inner and outer conductor. We found a geometric approach to suppressing multipacting. The most promising method was ripples in outer conductor. Ripples’ depth, width and gap were optimized. In shallow depth of 1 cm, electrons multiply, drift further, however they are stopped by 2 cm ripples. Width of 1 and 3 cm didn’t work as in 1 cm electrons emerge out of it, whereas, in 3 cm, they resonate and trap inside. A 2 cm wide was found good. Likewise, 2 cm gap was valuable. Finally, we find that ripples of 2 cm deep, 2 cm wide spaced by 2 cm completely suppressed multipacting, and were adopted for fabrication.

 
TU5PFP038 ILC 1.3 GHz Superconducting RF Technology Development Program at IHEP cavity, cryomodule, LLRF, niobium 906
 
  • J. Gao, S.Y. Chen, Y.L. Chi, J.P. Dai, J. Gu, M. Hou, K.X. Huang, T.M. Huang, S.P. Li, Z.Q. Li, Q. Ma, W.M. Pan, Y. Sun, G.W. Wang, Z.X. Xu, J. Yu, J.Y. Zhai
    IHEP Beijing, Beijing
  • L.Q. Liu, W.H. Lu, T.X. Zhao
    TIPC, BeiJing
 
 

Funding: NSFC 10525525


With the aim to develop 1.3 GHz superconducting radio-frequency (SCRF) technology in the frame of ILC collaboration, IHEP has started a program to build a SCRF Accelerating Unit. This unit contains a 9-cell 1.3 GHz superconducting cavity, a short cryomodule, a high power input coupler, a tuner, a low level RF system and a high power RF source, etc. This program also includes the SCRF laboratory upgrade, which will permit the unit to be built and tested at IHEP. We will use this unit as a horizontal test stand for many 9-cell cavities and other components (e.g. input couplers, tuners), as in Europe and North America. In this paper, we report the recent R&D status and the future plan of this program.

 
TU5PFP055 Hydroforming of Multi-Cell Niobium and NbCu-Clad Cavities cavity, niobium, cryogenics, electron 950
 
  • X. Singer, I. Jelezov, A. Matheisen, W. Singer
    DESY, Hamburg
  • P. Kneisel
    JLAB, Newport News, Virginia
 
 

Technological aspects of seamless tube fabrication and multi-cell cavity production by hydroforming will be discussed. Problems related to the fabrication of seamless cavities from bulk niobium are mainly solved. Several two cell- and three cell- niobium cavities have been produced by hydroforming at DESY. A 9-cell cavity of the TESLA shape has been completed from three sub-sections at company ZANON. The cavity was treated by electropolishing (EP) and successfully RF-tested. Two 3-cell units equipped with niobium beam pipes are being RF-tested after BCP surface treatment. The temperature mapping method with Jlab’s two-cell thermometry system is applied for performance analysis. It is of particular interest to compare the seamless cavity quench locations to those from standard cavities. The cryogenic test results and the T-mapping findings will be discussed. Of special interest is the combination of the seamless technique with NbCu cladding, i.e. the fabrication of cavity from bimetallic clad NbCu tube by hydroforming. Fabrication of single-cell and multi-cell NbCu clad cavities by hydroforming from bimetallic tubes is proven. Some test results will be presented.

 
TU5PFP065 FZJ HIPPI SC Triple-Spoke Cavity cavity, niobium, linac, vacuum 978
 
  • E.N. Zaplatin, R. Maier, M. Pap, R. Stassen, R. Tölle
    FZJ, Jülich
  • W. Behr, H. Glueckler, W. Guenther, J. Wolters
    Forschungszentrum Jülich GmbH, Institut fur Nuklearchemie (INC), Jülich
 
 

The paper describes the design, fabrication and first test results of the triple-spoke cavity (resonant frequency 352 MHz, beta=0.48) developed at Forschungszentrum Jülich in the frame of High Intensity Pulsed Proton Injector project. The cavity has 5 cm diameter beam aperture, a transverse radius of 21.7 cm and the whole length of 78 cm. An initial wall thickness of niobium sheets used for cavity fabrication was around 4 mm. The RF cavity design has been adapted to two main goals - the simplest technology of cavity manufacture and for the prime goal of the project to achieve the best possible structural parameters (Lorenz force frequency shift and a resonant frequency pressure dependence). Intense cavity structural analyses have been conducted and the further prospectives on cavity developments are also presented. Construction of the niobium cavity prototype has been completed, the cavity has been chemically processed. Results of initial cold test are discussed.

 
TU5PFP066 IFMIF Superconducting beta=0.094 Half-Wave Resonator Design cavity, multipactoring, insertion, linac 981
 
  • E.N. Zaplatin
    FZJ, Jülich
  • P. Bosland, P. Bredy, N. Grouas, P. Hardy, J. Migne, A. Mosnier, F. Orsini, J. Plouin
    CEA, Gif-sur-Yvette
 
 

The driver of the International Fusion Material Irradiation Facility (IFMIF) consists of two 125 mA, 40 MeV cw deutron accelerators. A superconducting option for the 5 to 40 MeV linac is based on Half-Wave Resonators (HWR) has been choosen. The first cryomudule should contain 8 HWR's with resonant frequency of 175 MHz and beta=v/c=0.094. The paper describes RF design of half-wave length resonator. The requirents on high power coupler define its installation in the cavity central region. Few options of cavity tune were investigated, the capacitive tuner installed opposite to the coupler port have been accepted. The cavity structural analyses have been conducted and cavity stiffening has been worked out.

 
TU5PFP079 A Status Report on the Advanced Photon Source 2-MW DC Resistive Load power-supply, klystron, high-voltage, impedance 1011
 
  • G. Trento, D. Horan, E. Swetin, G.J. Waldschmidt
    ANL, Argonne
 
 

Funding: Work supported by U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


The redesign, construction, and high-power testing of a 95-kV DC, 2MW water-cooled resistive load has been completed. This load was built and installed to test and troubleshoot the Advanced Photon Source (APS) 352-MHz high –voltage klystron power supplies. The original resistive load*,** was modified to enhance and improve the load performance .In this paper, we describe the redesign of the DC load, report on the recent test results, and discuss it’s performance improvements.


*D. Horan et al., “A 2-Megawatt Load for Testing High Voltage DC Power Supplies”.
** D. Horan et al., “Performance of a 2-Megawatt High Voltage test Load”.

 
TU5PFP084 Multi-MW K-Band 7th Harmonic Multiplier for High-Gradient Accelerator R&D cavity, gun, electron, coupling 1026
 
  • N. Solyak, V.P. Yakovlev
    Fermilab, Batavia
  • J.L. Hirshfield, G.M. Kazakevich
    Omega-P, Inc., New Haven, Connecticut
  • M.A. LaPointe
    Yale University, Physics Department, New Haven, CT
 
 

Funding: Sponsored in part by US Department of Energy, Office of High Energy Physics.


A preliminary design is presented for a two-cavity 7th harmonic multiplier, intended as a high-power RF source for use in experiments aimed at developing high-gradient structures for a future collider. The harmonic multiplier is to produce power in K-band using as an RF driver an XK-5 S-band klystron (2.856 GHz). The device is to be built with a TE111 rotating mode input cavity and interchangeable output cavities, a principal example of which is a TE711 mode cavity running at 19.992 GHz. Design of the harmonic multiplier is described that uses a 250 kV, 20 A injected laminar electron beam. With 10 MW of S-band drive power, 4.7 MW of 20-GHz output power is predicted. Details are described of the gun beam optics, beam dynamics in the RF system, and of the magnetic circuit. The theory of an azimuthally distributed coupler for the output cavity is presented, as well as the conceptual design of the entire RF circuit.

 
TU5PFP093 Low Beam Voltage, 10 MW, L-Band Cluster Klystron cavity, gun, cathode, klystron 1051
 
  • V.E. Teryaev
    BINP SB RAS, Novosibirsk
  • J.L. Hirshfield
    Yale University, Physics Department, New Haven, CT
  • S. Kazakov
    KEK, Ibaraki
  • V.P. Yakovlev
    Fermilab, Batavia
 
 

Funding: Sponsored in part by US Department of Energy, Office of High Energy Physics.


Conceptual design of a multi-beam klystron (MBK) for ILC and Project X application is presented. The chief distinction between the MBK design and existing 10-MW MBK’s is the low operating voltage of 60 kV. There are at least four compelling reasons that justify development of a low-voltage MBK, namely (i) no pulse transformer would be required; (ii) no oil tank would be required for the tube socket; (iii) modulator would be a compact 60-kV IGBT switching circuit. The proposed klystron consists of four clusters that contain six beams each. The tube has common input and output cavities for all 24 beams, and individual gain cavities for each cluster. A closely related optional configuration for a 10 MW tube would involve a design having four totally independent cavity clusters and four 2.5 MW output ports, all within a common magnetic circuit. This option has appeal because the output waveguides would not require a controlled atmosphere and because it would be easier to achieve phase and amplitude stability as required in individual SC cavities.

 
TU5RFP007 NSLS-II Booster Acceptance Studies booster, injection, kicker, lattice 1099
 
  • R.P. Fliller, W. Guo, R. Heese, Y. Li, T.V. Shaftan
    BNL, Upton, Long Island, New York
 
 

The NSLS II is a state of the art 3 GeV synchrotron light source being developed at BNL. The injection system will consist of a 200 MeV linac and a 3GeV booster synchrotron. The injection system must supply 7.3nC every minute to satisfy the top off requirements. A large booster acceptance is neccessary to have a high booster injection efficiency and alleviate the requirements on linac gun. We also anticipate transverse stacking of bunches in the booster to increase the amount of charge that can be delivered. We present studies of the anticipated booster stay clear including lattice errors and the ramifications for injection efficiency and transverse stacking.

 
TU5RFP011 Top-Off Safety Analysis for NSLS-II dipole, electron, radiation, injection 1111
 
  • Y. Li, W.R. Casey, R. Heese, H.-C. Hseuh, P.K. Job, S. Krinsky, B. Parker, T.V. Shaftan, S. Sharma
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by U.S. DOE, Contract No.DE-AC02-98CH10886


Top-off injection will be adopted in NSLS-II. To ensure no injected beam can pass into experimental beamlines with open photon shutters during top-off injection, simulation studies for possible machine fault scenarios are required. We compare two available simulation methods, backward (H. Nishimura-LBL) and forward tracking (A. Terebilo-SLAC). We also discuss the tracking settings, fault scenarios, apertures and interlocks considered in our analysis.

 
TU5RFP013 Dynamic Response and Filtering Effects of a Light Source Accelerator Ring Structure site, ground-motion, lattice, storage-ring 1117
 
  • N. Simos, M. Fallier
    BNL, Upton, Long Island, New York
 
 

Vibration stability in third generation light sources such as the 3 GeV NSLS II under construction at BNL and which are aiming at high brightness and extremely small photon beam sizes is paramount. Movement of the magnetic elements of the accelerator lattice, and in particular when uncorrelated, will induce jitter in the beam and degrade the machine performance. The accelerator lattice response is coupled with the ring structure which in turn interacts with the site and the ground vibration field that characterizes it. Therefore, understanding this dynamic coupling between the accelerator ring structure and the site and the “filtering” effect of the interaction on both the amplitude and the spectral characteristics of the ground vibration is central towards establishing the response of the lattice. In this study, the site-ring dynamic interaction is evaluated based on the NSLS II design and site conditions using a state-of-the-art 3-D wave propagation and scattering analysis model. The study is augmented with an extensive array of measurements at the selected site as well as field studies at similar operating light source facilities.

 
TU5RFP014 Numerical Treatment of Moving Loads Affecting the Stability of NSLS II Light Source Accelerator site, ground-motion, acceleration, synchrotron 1120
 
  • N. Simos, M. Fallier, T.F. Joos
    BNL, Upton, Long Island, New York
 
 

Cultural noise generated within or in the proximity of a light source facility aiming to achieve stability levels of just tens of nanometers in the electron beam and extremely small photon beams in special experimental lines could be a limiting factor towards achieving the performance goals. While operating systems within the facility are more readily identifiable as sources of vibration and cause of instabilities and they tend to be of deterministic nature so appropriate action can be taken to minimize their impact, moving-type loads such as traffic in the general vicinity or within the bounds of the accelerator facility are more of a stochastic nature and require a different approach in assessing its impact on the synchrotron facility. In this study the effect of such loads which poses both stochastic elements and a complex spectrum on the stability performance goals of the NSLS II synchrotron and its vibration-sensitive experimental lines is addressed prior to the construction of the facility. This is achieved through the synergy of a comprehensive numerical model and an array of recorded field data.

 
TU5RFP015 Model for Addressing NSLS II Lattice Response to Random, Stationary Vibration lattice, site, ground-motion, photon 1123
 
  • N. Simos
    BNL, Upton, Long Island, New York
 
 

The extremely small photon beam dimensions of NSLS II impose challenging requirements on the e-beam orbital stability in the 6-D phase space. The electron beam orbit at the photon source locations must remain within a few hundred nanometer window for a wide frequency band. The beam orbit movement is coupled to the movement of the magnetic elements in the lattice which are itself coupled to the ring-building structure. While the vibration exciting the ring structure consists of deterministic and stochastic noise, it is the high frequency random, uncorrelated part that has the largest impact on the residual beam orbit movement as it is most difficult to control by fast orbit feedback. In this study, an analytical model is employed to quantify lattice displacement and beam orbit jitter for the expected conditions of NSLS II. The dynamic interaction of the ring supporting the lattice with the stationary ground vibration is addressed using a 3-D model of wave-structure interaction. Cross transfer functions linking ground vibration with the ring and magnetic lattice for various stochastic parameters are deduced leading to a multi-degree of freedom cross-spectral density of the lattice.

 
TU5RFP030 Universal Mode Operation of the BESSY II UE112 APPLE Undulator undulator, multipole, polarization, electron 1162
 
  • J. Bahrdt, W. Frentrup, A. Gaupp, M. Scheer
    HZB, Berlin
 
 

The UE112 APPLE undulator operated at BESSY II covers the low photon energies down to the visible regime. Below 100eV the state of polarization is significantly modified by the optical components of the beamline. Moving independently three magnet rows of the APPLE undulator (universal mode) any state of polarization can be produced which permits the compensation of the beamline effects. Thus, circularly polarized light can be provided at the experiment. The dynamic multipoles of the universal mode can be compensated with flat wires which are glued onto the vacuum chamber. Simulations and first experiments with the electron beam related to the dynamic multipoles and their compensation are presented.

 
TU5RFP034 Design Study of a Dedicated Beamline for THz Radiation Generation at the SPARC Linac radiation, electron, target, laser 1168
 
  • M. Boscolo, M. Castellano, E. Chiadroni, M. Ferrario
    INFN/LNF, Frascati (Roma)
  • P. Calvani, S. Lupi, A. Nucara
    Università di Roma I La Sapienza, Roma
  • B. Marchetti
    INFN-Roma II, Roma
  • A. Perucchi
    ELETTRA, Basovizza
  • V. Petrillo
    Universita' degli Studi di Milano, Milano
  • A.R. Rossi
    Istituto Nazionale di Fisica Nucleare, Milano
 
 

A feasibility study for a dedicated beamline for a THz radiation source at SPARC is discussed. A radiofrequency electron gun followed by a compressor can generate trains of THz sub-picosecond electron pulses by illuminating the photocathode with a comb laser pulse. This structure of the beam can be used to produce coherent radiation. The quality of the coherent spectrum emitted by a comb beam is tightly connected to the electron micro-bunches lengths and to micro-pulses inter-distance. Beam dynamics studies are summarized here and compared to a conventional single bunch case, optimized for the THz radiation generation. The dynamics is studied within the SPARC system with the PARMELA code and with the RETAR code for the evaluation of the radiation.

 
TU5RFP043 Design of a 250 MeV, X-Band Photoinjector Linac for a Precision Compton-Scattering Based Gamma-Ray Source emittance, electron, linac, gun 1186
 
  • S.G. Anderson, F. Albert, C.P.J. Barty, D.J. Gibson, F.V. Hartemann, D.P. McNabb, M. J. Messerly, B. Rusnak, M. Shverdin, C. Siders
    LLNL, Livermore, California
  • S.G. Tantawi, A.E. Vlieks
    SLAC, Menlo Park, California
 
 

Funding: This work performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344.


We present a compact, X-band, high-brightness accelerator design suitable for driving a precision gamma-ray source. Future applications of gamma-rays generated by Compton-scattering of laser and relativistic electron beams place stringent demands on the brightness and stability of the incident electron beam. This design identifies the beam parameters required for gamma-ray production, including position, and pointing stability. The design uses an emittance compensated, 11.4 GHz photo-gun and linac to generate 400 pC, 1-2 mm-mrad electron bunches at up to 250 MeV and 120 Hz repetition rate. The effects of jitter in the photo-cathode laser and RF power system are analyzed as well as structure and optic misalignments and wakefields. Finally, strategies for the mitigation of on-axis bremsstrahlung noise are discussed.

 
TU5RFP052 Experimental Characterization of a SASE FEL in the Exponential Gain and Saturation Regimes FEL, undulator, electron, emittance 1204
 
  • X.J. Wang, Y. Hidaka, J.B. Murphy, B. Podobedov, H.J. Qian, S. Seletskiy, Y. Shen, X. Yang
    BNL, Upton, Long Island, New York
  • B. Hafizi
    Icarus Research, Inc., Bethesda, Maryland
  • J. Penano, P. Sprangle
    NRL, Washington, DC
 
 

The NSLS Source Development Laboratory (SDL) has been a world leader in the development of laser seeded free electron lasers (FEL). Recently we initiated an experimental program to investigate a Self-Amplified Spontaneous Emission (SASE) FEL in both the exponential gain and the saturation regimes. We have experimentally demonstrated the saturation of a SASE FEL in the visible to near IR. The experimental characterization of the transverse and spectral properties of the SASE FEL along the undulator for a uniformed and tapered undulator will be presented. In addition, an efficiency enhancement concept for a SASE FEL, which involves a step wiggler taper in the exponential gain regime prior to trapping, will be presented. Simulations of the SASE FEL processes will employ the GENESIS FEL code.

 
TU5RFP053 Efficiency and Spectrum Enhancement in a Tapered Free-Electron Laser Amplifier undulator, laser, electron, FEL 1207
 
  • X.J. Wang, D.A. Harder, J.B. Murphy, H.J. Qian, Y. Shen, X. Yang
    BNL, Upton, Long Island, New York
  • H. Freund, W.H. Miner
    SAIC, McLean
 
 

Funding: This work is supported in part by the Office of Naval Research (ONR), the Joint Technology Office, and U.S. Department of Energy (DOE) under contract No. DE-AC02-98CH1-886.


We report the first experimental characterization of efficiency and spectrum enhancement in a laser-seeded free-electron laser (FEL) using a tapered undulator. Output and spectra in the fundamental and 3rd harmonic were measured versus distance for uniform and tapered undulators. With a 4% field taper over 3 m, a 300% (50%) increase in the fundamental (3rd harmonic) output was observed. A significant improvement in the spectra with the elimination of side-bands was observed for the first time using a tapered undulator. The experiment is in good agreement with predictions using the MEDUSA simulation code.

 
TU5RFP077 Microbunching Instability Modeling in the SPARX Configurations laser, electron, bunching, undulator 1266
 
  • C. Vaccarezza, M. Ferrario, A. Marinelli
    INFN/LNF, Frascati (Roma)
  • L. Giannessi, C. Ronsivalle
    ENEA C.R. Frascati, Frascati (Roma)
  • M. Migliorati
    Rome University La Sapienza, Roma
  • M. Venturini
    LBNL, Berkeley, California
 
 

The modeling of the microbunching instability has been carried out for the SPARX FEL accelerator, two configurations have been considered and compared: hybrid compression scheme (velocity bunching plus magnetic compressor) and purely magnetic. The effectiveness of a laser heather in reducing this instability drawbacks on the electron beam quality has also been exploited. Analytical predictions and start to end simulation results are reported in this paper.

 
TU6PFP009 Designing Integrated Laser-Driven Ion Accelerator Systems for Hadron Therapy at PMRC (Photo Medical Research Center) laser, ion, proton, hadron 1309
 
  • H. Sakaki, P.R. Bolton, T. Hori, S. Kawanishi, M. Nishiuchi
    JAEA, Tokai-mura
  • H. Daido
    JAEA/Kansai, Kyoto
  • Y. Iseki, T. Yoshiyuki
    Toshiba, Tokyo
  • A. Noda, H. Souda
    Kyoto ICR, Uji, Kyoto
  • K. Sutherland
    Hokkaido University, Sapporo
 
 

The cancer treatment with hadron beams continues to be made as hadron treatment facilities are being developed around the globe with state-of-the-art accelerator technology. The generation of energetic protons and ions from laser-plasma interactions, has made laser-driven hadron radiotherapy a subject of strong interest. Proton bunches with high peak current and ultralow emittance are typical of ultrafast laser-foil interactions. However, these bunches also exhibit large divergence and energy spread. Photo Medical Research Center (PMRC) of JAEA was recently established to address the challenge of the laser-driven ion accelerator development for hadron therapy. Our mission at PMRC is to develop integrated, laser-driven ion accelerator systems (ILDIAS) that demonstrate desired beam characteristics for such therapy. We used the Phase and Radial Motion in Ion Linear Accelerators (PARMILA) design software which was originally developed as a numerical tool to design and simulate beam performance. This report will discuss beam specifications of laser-driven ion accelerators using PARMILA.

 
TU6PFP011 Preliminary Results of Sample Activation Measurement Using a HPGe Detector for the Nano Particle Fabrication by Proton Beam proton, target, radiation, radioactivity 1315
 
  • K. R. Kim, J.-H. Jang, M.H. Jung, H.O. Kim, C.W. Lee
    KAERI, Daejon
  • G.S. Chai
    Samsung SDI Co. Ltd., Gyeonggi-do
  • H.J. Kim
    Kyungpook National University, Daegu
  • M.K. Min
    SAMSUNG SDI CO. LTD, Gyeonggi-do
 
 

Funding: This work was performed as a part of the Proton Engineering Frontier Project supported by the Ministry of Education, Science and Technology of Korea.


The sample activation during proton beam irradiation sometimes interrupt the measurement and investigation of the instant changes of the samples after irradiation. During the experiments for nano particle fabrications with ~35MeV and ~20uA, we found that the samples was highly activated after the proton beam irradiation. To investigate the source of the rdadiation from the samples, we measured the energy spectrum of gamma ray using HPGe spectroscopy. The results was compared to the calculated results by the MCNP code simulation. The sample was small amount of heavy metal dispersed in enthanol in the beaker made of quartz.

 
TU6PFP012 Extra Dose Reduction by Optimizing RF-KO Slow-Extraction at HIMAC ion, controls, extraction, betatron 1318
 
  • K. Mizushima, T. Furukawa, Y. Iwata, K. Noda, S. Sato, T. Shirai
    NIRS, Chiba-shi
  • T. Fujisawa, H. Uchiyama
    AEC, Chiba
 
 

A 3D scanning method gated with patient's respiration has been developed for the HIMAC new treatment facility. In the scanning irradiation, the RF-KO slow-extraction method has been used, because of the quick response to beam on/off from the synchrotron. However, a small amount of beam remained just inside the separatrix is extracted just before turning on the transverse RF field, which brings the extra dose. We proposed to apply another transverse RF-frequency component matched with the betatron frequency of the particles in the vicinity of the stopband, in addition to the original transverse RF field for the RF-KO slow-extraction. Using the proposed method, the particles just inside the separatrix, which cause the extra dose, can be selectively extracted during the irradiation; as a result, the extra dose can also be reduced. The validity of this approach has been verified by the simulation and the measurement with the non-distractive 2D beam profile monitor. We will report the result of this approach.

 
TU6PFP016 Pinpoint keV X-Ray Imaging for X-Ray Drug Delivery System scattering, laser, radiation, electron 1328
 
  • M. Uesaka
    The University of Tokyo, Nuclear Professional School, Ibaraki-ken
  • R. Kuroda, K. Yamada
    AIST, Tsukuba, Ibaraki
  • K. Mizuno, A. Mori, T. Natsui, H. Taguchi, J.D. Trono
    University of Tokyo, Tokyo
  • N. Yusa
    Tohoku University, Graduate School of Engineering, Sendai
 
 

In X-ray Drug Delivery System, anticancer drugs containing Pt, such as cisplatin and dachplatin, and Au colloid contrast agent are surrounded by polymers (micelle, PEG (polyethylene glycol), etc.).Ttheir sizes are controlled to be 20-100 nm. Since holes of capillary to organ are as large as 100 nm in only cancer, those large particles can be accumulated in cancer effectively. That is called as EPR (Extended Penetration and Retention effect). We have observed the distribution of Pt of dachplatin-micelle in cancer of mouse’s pancreas by X-ray fluorescence analysis using 10 μm pinpoint 15 keV X-ray by SPring8. Further, in-vitro- and in-vivo-experiments of Au colloid PEG are under way. It is expected to be used as contrast agent for dynamic tracking treatment for moving cancer. Imaging properties for polychromatic X-rays from X-ray tube and monochromatic Compton source are numerically analyzed and discussed. We continue to analyze radiation enhancement by Auger electrons and successive characteristic X-rays and its toxic effect to cancer.

 
TU6PFP018 Ultrafast Electron Diffraction System at the NSLS SDL electron, solenoid, gun, emittance 1333
 
  • Y. Hidaka, C.C. Kao, J.B. Murphy, S. Pjerov, B. Podobedov, H.J. Qian, S. Seletskiy, Y. Shen, X.J. Wang, X. Yang
    BNL, Upton, Long Island, New York
 
 

Ultrafast electron diffraction (UED) is a promising technique that allows us to observe a molecular structure transition on a time scale on the order of femtoseconds. The UED has several advantages over the competing technology, X-Ray Free Electron Laser (XFEL) in terms of its compactness, 6 orders of magnitude larger cross section, and less damaging ability to the samples being probed. Present state-of-the-art UED systems utilize subrelativistic electron bunches as the probing beam. With such low energy, however, the number of electrons in the bunch must be significantly decreased for a short bunch length (~100 fs) due to space charge effects. This limits the detection capability of such keV UED devices. To overcome this issue, a UED system using an MeV electron beam has been proposed, and designed at Source Development Laboratory (SDL) in National Synchrotron Light Source (NSLS) at Brookhaven National Laboratory (BNL). A detailed performance analysis of this system using the particle tracking code, GPT, from the photoinjector cathode to the detector, will be presented, as well as the status of the commissioning of our UED system.

 
TU6PFP029 Neutron Spallation Studies for an Accelerator Driven Subcritical Reactor neutron, target, proton, scattering 1351
 
  • C. Bungau
    Manchester University, Manchester
  • R.J. Barlow
    UMAN, Manchester
  • A. Bungau, R. Cywinski
    University of Huddersfield, Huddersfield
 
 

Nuclear power production can benefit from the development of more comprehensive alternatives for dealing with long-term radioactive waste. One such alternative is an accelerator-driven subcritical reactor (ADSR) which has been proposed for both energy production and for burning radioactive waste. Here we investigate the effects of the size of the ADSR spallation target on the total neutron yield integrated over the neutron energy and emission angle. The contribution to the total neutron yield from the (n, xn) neutron interactions is evaluated at proton beam energies between 0.4 and 2 GeV. Calculations have been carried out with the GEANT4 simulation code using the Liege intranuclear cascade model and the results are compared to the the LAHET/MCNP code package predictions.

 
TU6PFP031 Research on a Terahertz Coherent Transition Radiation Source Based on Ultrashort Electron Beam radiation, target, electron, vacuum 1357
 
  • W. Liu, Y.-C. Du, W.-H. Huang, C.-X. Tang, D. Wu
    TUB, Beijing
 
 

The preliminary experiments and three-dimensional (3D) particle-in-cell (PIC) simulations of terahertz (THz) coherent transition radiation (CTR) performed at the Accelerator Laboratory of Tsinghua University are reported in this paper. THz radiation is generated from the interactions of Titanium foil with the ultrashort electron beam produced by the photocathode RF gun. The frequency and power of radiation are measured with the Martin-Pupllet interferometer and Gollay Cell detector, respectively. The radiation characteristics depending on the foil properties are preliminarily studied with the experiments and PIC simulations. On the other hand, the distribution of radiation field pattern and energy are studied by numerical calculated, and those results are in agreement with the PIC simulations.

 
TU6PFP038 Studies of High Energy Density Matter Using Intense Ion Beams at FAIR at Darmstadt: The HEDgeHOB Collaboration ion, target, heavy-ion, antiproton 1366
 
  • N.A. Tahir
    GSI, Darmstadt
  • C. Deutsch
    Laboratoire de Physique des Gaz et des Plasmas, Universite Paris-Sud, Orsay
  • V.E. Fortov, I. Lomonosov, A. Shutov
    IPCP, Chernogolovka, Moscow region
  • D.H.H. Hoffmann
    TU Darmstadt, Darmstadt
  • R. Piriz
    Universidad de Castilla-La Mancha, Ciudad Real
 
 

Studies of High Energy Density (HED) states in matter is one of the recently proposed important applications of intense particle beams. GSI Darmstadt is worldwide famous due to its unique accelerator facilities. Construction of the new accelerator FAIR, will enhance these capabilities many fold. During the past years, extensive theoretical work has been carried out to propose future HED physics experiments that could be carried out at FAIR. It is expected that the new heavy ion synchrotron, SIS100, will deliver a uranium beam with 1012 uranium ions that will be delivered in a single bunch, 50 – 100 ns long. Circular, elliptic and annular focal spots can be generated that will allow one to perform different type of HED physics experiments. This work has shown that using a special technique, named HIHEX, one may access those areas of the phase diagram that have never been accessed before. Using another experimental configuration, LAPLAS , it will be possible to generate physical conditions that are expected to exist in the interiors of the giant planets. Material properties under dynamic conditions can also be studied using a third experimental set up.

 
TU6PFP039 Material Recognition by Means of Different Bremsstrahlung Beams: Is that Really Possible? electron, linac, scattering, target 1369
 
  • L. Auditore
    INFN - Gruppo Messina, S. Agata, Messina
  • L. Auditore, R.C. Barnà, D. Loria, E. Morgana, A. Trifirò, M. Trimarchi
    Università di Messina, Messina
  • M. Carpinelli
    INFN-Cagliari, Monserrato (Cagliari)
  • A. Franconieri, M. Gambaccini
    INFN-Ferrara, Ferrara
 
 

At the Dipartimento di Fisica, Università di Messina, an X-ray source based on a 5 MeV electron linac has been designed. By means of the MCNP-4C2 code, several simulations have been performed to evaluate if the source can be used as a NDT device for material recognition purposes. In particular, being able to vary the electron beam energy for producing bremsstrahlung beams with different absorption, X-ray transmission through several materials and for different X-ray beams energy has been studied. First results have shown the capability of the system to distinguish dissimilar materials by properly choosing the X-ray beam end-point energy and processing the obtained transmission values. Since the uncertainties level in the material identification could be improved differentiating the response of the imaging system, a theoretical study has been performed to evaluate how X-ray beams obtained with different end-point energies, and eventually transmitted by properly chosen filters, are absorbed by different scintillators. The obtained results will be presented and discussed in order to give indications on the real chance to use the designed device for material recognition purposes.

 
TU6PFP049 Coherent Terahertz Radiation Emitted by Sub-Picosecond Electron Bunches in a Magnetic Chicane radiation, electron, polarization, dipole 1391
 
  • M.P. Dunning, G. Andonian, A.M. Cook, E. Hemsing, A.Y. Murokh, S. Reiche, J.B. Rosenzweig, D. Schiller
    UCLA, Los Angeles, California
  • M. Babzien, K. Kusche, V. Yakimenko
    BNL, Upton, Long Island, New York
 
 

Coherent radiation emitted by relativistic electron bunches traversing the edge regions of dipole magnets in a chicane bunch compressor was extracted and transported for measurement, using a dedicated terahertz beamline at the Accelerator Test Facility (ATF) at Brookhaven National Laboratory (BNL). Measurements include frequency spectrum and polarization of the radiation. The measurements are compared to predictions from QUINDI, a new simulation code developed at UCLA to model radiation emitted by charged particles in bending systems. Simulations and measurements indicate that because of interference of radiation from the two magnet edges, the edge radiation is suppressed at long wavelengths. In addition to being a source of broadband terahertz radiation, the system is also used as a non-invasive, single-shot, relative bunch length diagnostic to monitor compression in the chicane.

 
TU6PFP051 Development and Optimisation of the Muon Target at the ISIS-RAL Muon Facility target, proton, beam-losses, vacuum 1397
 
  • A. Bungau, R. Cywinski
    University of Huddersfield, Huddersfield
  • J.S. Lord
    STFC/RAL, Chilton, Didcot, Oxon
 
 

The pulsed muon channel of the ISIS facility at Rutherford Appleton Laboratory has been successfully commissioned and operated for many years as a tool for MuSR studies in condensed matter research. At the present time, the graphite target, of dimensions 50*50*7 mm oriented at 45 degrees to a proton beam of 800 MeV energy, gives 16000 surface muons per double proton pulse passing through the entrance aperture of the aluminium window which separates the muon beamlines from the main proton beam. Potential improvements to the target geometry, and optimisation of the design and estimated performance of the muon target are presented in this paper.

 
TU6PFP052 GEANT4 Simulations of the ISIS Muon Target at Rutherford Appleton Laboratory target, proton, neutron, hadron 1400
 
  • A. Bungau, R. Cywinski
    University of Huddersfield, Huddersfield
  • J.S. Lord
    STFC/RAL, Chilton, Didcot, Oxon
 
 

MuSR science requires the availability of intense beams of polarised positive muons. At the ISIS pulsed muon facility at Rutherford Appleton Laboratory the muons are generated from a low Z thin slab graphite target inserted in the proton beam. We report on the use of the Monte Carlo simulation code Geant4 in simulations of the performance of the current muon target. The results are benchmarked against the experimental performance of the target.

 
TU6PFP054 Simulations of Longitudinal Phase Space Painting for the CSNS RCS Injection beam-losses, injection, synchrotron, proton 1403
 
  • L. Liu, J. Qiu, J. Tang, T. Wei
    IHEP Beijing, Beijing
 
 

China Spallation Neutron Source (CSNS) is a high power proton accelerator-based facility. Uncontrolled beam loss is a major concern in designing the high power proton accelerators to control the radio-activation level. For the Rapid Cycling Synchrotron (RCS) of the CSNS, the repetition frequency is too high for the longitudinal motion to be fully adiabatic. Significant beam loss happens during the RF capture and initial acceleration. To reduce the longitudinal beam loss, phase space painting is used in the RCS injection. This paper presents detailed simulation studies on the longitudinal motion in the RCS by using the ORBIT code, which include different beam chopping factors, momentum offsets, injection times and RF voltage patterns. With a trade-off between the longitudinal beam loss and transverse incoherent tune shift that will also result in beam losses, optimized longitudinal painting schemes are obtained.

 
TU6PFP056 Longitudinal Painting Schemes for H- Charge Exchange Injection into the PS2 injection, synchrotron, bunching, linac 1409
 
  • C. Carli, M. Benedikt, S. Hancock
    CERN, Geneva
  • V. Knuenz, I. Vonderhaid
    TU Vienna, Wien
 
 

Minimization of direct space charge tune shift at injection into the PS2 is important for the reduction of beam losses. A determining parameter for the tune shift is the bunching factor, defined as mean current over peak current for one RF period. Various longitudinal painting schemes for PS2 injection, all based on synchrotron motion, have been studied with respect to the resulting bunching factors. In particular, schemes using the SPL high-frequency chopper and different energy-spreads and offsets of the incoming beam as well as SPL beam energy modulations on have been simulated with the ESME code.

 
TU6PFP059 Numerical Studies of High-Intensity Injection Painting for Project X space-charge, injection, proton, linac 1418
 
  • A.I. Drozhdin, D.E. Johnson, L.G. Vorobiev
    Fermilab, Batavia
 
 

Injection painting enables the mitigation of space charge and stability issues, and may be indispensable for the Project-X at Fermilab, delivering high-intensity proton beams to HEP experiments. Numerical simulations of multi-turn phase space painting have been performed for the FNAL Recycler Ring, including a self-consistent space charge model, lattice nonlinearities, H- stripping, particle loss and foil heating. Different painting waveforms were studied to build a uniform (KV-like distribution) and other phase space distributions.

 
TU6PFP067 Beam Loss Issues Connected to the Foil Scattering: Estimation vs. Measurement at the RCS of J-PARC injection, beam-losses, scattering, insertion 1442
 
  • P.K. Saha, N. Hayashi, H. Hotchi, K. Yamamoto, M. Yoshimoto
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  • Y. Irie
    KEK, Ibaraki
  • T. Toyama
    J-PARC, KEK & JAEA, Ibaraki-ken
 
 

The beam loss issues connected to the nuclear scattering together with the multiple Coulomb scattering at the charge-exchange foil during the multi-turn injection has been studied in detail for the RCS (Rapid Cycling Synchrotron) of J-PARC (Japan Proton Accelerator Research Complex). Recently, during the beam commissioning of RCS, some experimental data related to such issue has been taken and thus a comparison of the measured beam loss to the estimated one is reported in this paper. When the beam loss from such a source is unavoidable, a realistic estimation is quite important for a fair design of the injection system and the vicinity in order to reduce especially, the uncontrolled beam loss.

 
TU6PFP068 Longitudinal Painting Studies in the J-PARC RCS injection, bunching, cavity, beam-losses 1445
 
  • F. Tamura, K. Hasegawa, M. Nomura, A. Schnase, T. Shimada, H. Suzuki, M. Yamamoto
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  • K. Hara, C. Ohmori, M. Tada, M. Yoshii
    KEK/JAEA, Ibaraki-Ken
 
 

In the J-PARC RCS, we employ the longitudinal painting methods, the momentum offset injection method and applying the second harmonic RF voltages, to increase the bunching factor so that the space-charge tune shift is reduced. By the dual-harmonic operation with wide-band MA loaded cavities, in which each single cavity is driven by a superposition of the fundamental and the second harmonic RF signals, we can generate a large amplitude second harmonic RF voltage without extra cavities for the second harmonic RF. We present the results of the beam tests for the longitudinal painting in the J-PARC RCS. Also, we present the beam behavior at very high beam power.

 
TU6PFP070 The Beam Dynamics Design for J-PARC Linac Energy Upgrade linac, quadrupole, cavity, klystron 1451
 
  • M. Ikegami
    KEK, Ibaraki
  • H. Ao
    JAEA/LINAC, Ibaraki-ken
  • T. Morishita, H. Sako, Y. Yamazaki
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
 
 

The output energy of J-PARC linac is planned to be upgraded from 190 MeV to 400 MeV by adding an ACS (Annular Coupled Structure linac) section. The ACS is a variety of coupled-cavity structure linac newly devised for former JHP (Japan Hadron Project), and its original beam dynamics design for J-PARC was presented in LINAC02 [M. Ikegami et. al., in Procs. of LINAC02, p. 629]. Extensive R&D studies have been conducted since then to establish the feasibility of ACS, where four ACS modules have been fabricated and successfully high-power tested. In parallel, the beam dynamics design of the ACS has been further optimized to reflect the experience obtained in the R&D studies and reduce the cost for mass production. In this paper, the revised beam dynamics design of the J-PARC ACS is presented with some simulation results with a particle simulation code.

 
TU6PFP082 Baseline Design for the ESS-Bilbao Superconducting Proton Accelerator cavity, linac, acceleration, SRF 1482
 
  • F.J. Bermejo
    Bilbao, Faculty of Science and Technology, Bilbao
  • I. Bustinduy
    ESS Bilbao, Bilbao
  • J. Lucas
    Elytt Energy, Madrid
 
 

Funding: ESS-Bilbao Consortium


A baseline design for the proton linear accelerator as proposed by the European Spallation Source-Bilbao bid to host the installation (ESS-B) is here described. The new machine concept incorporates advances which have been registered within high power accelerators during the last decade. The design of such a new accelerator layout heavily relies upon low-beta superconducting spoke resonators which are already under development.

 
TU6PFP084 A 15 MeV Accelerator Scheme Based on a DC Photo-Injector and a RF Superconducting Linac vacuum, electron, target, cathode 1488
 
  • D. Guilhem, J.-L. Lemaire
    CEA, Arpajon
 
 

A 15 MeV accelerator scheme based on a DC photo-injector and a RF superconducting linac has been proposed as a new facility for radiography applications. The design of a 15 MeV, 2 kA peak current, electron accelerator for the DEINOS project is presented The beam operating condition is a limited number of bunches up to twenty electron micro-pulses of 100 ps time duration and 200 nC bunch charge emitted at 352 MHz repetition rate from a Cs2Te photocathode and accelerated to 2.5 MeV in the DC diode before injection into a superconducting linac. A general description of the main accelerator components and the beam dynamics simulations are presented. The overall beam dynamics simulation process based on LANL POISSON-SUPERFISH and PARMELA codes and the results will be reviewed.

 
TU6PFP090 High-Intensity Demonstrations in the J-PARC 3-GeV RCS injection, beam-losses, space-charge, linac 1504
 
  • H. Hotchi, N. Hayashi, Y. Hikichi, S. Hiroki, J. Kamiya, K. Kanazawa, M. Kawase, M. Kinsho, M. Nomura, N. Ogiwara, R. Saeki, P.K. Saha, A. Schnase, T. Shimada, Y. Shobuda, K. Suganuma, H. Suzuki, H. Takahashi, T. Takayanagi, O. Takeda, F. Tamura, N. Tani, T. Togashi, T. Ueno, M. Watanabe, Y. Watanabe, K. Yamamoto, M. Yamamoto, Y. Yamazaki, H. Yoshikawa, M. Yoshimoto
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  • A. Ando
    LASTI, Hyogo
  • H. Harada
    Hiroshima University, Graduate School of Science, Higashi-Hiroshima
  • K. Hasegawa, Y. Irie, C. Ohmori, M. Yoshii
    KEK, Ibaraki
  • K. Satou, Y. Yamazaki
    J-PARC, KEK & JAEA, Ibaraki-ken
 
 

The beam commissioning of the J-PARC 3-GeV RCS started in October 2007. The initial machine parameter tuning and underlying beam studies were completed in February 2008 through various beam dynamics measurements, such as optical functions, turn-by-turn beam positions, and transverse and logitudinal beam profiles. Now the RCS is in transition from the first commissioning phase to the next challenging stage and our efforts hereafter will be focused on higher beam power operations. In this paper, we describe experimental results obtained in the high intensity demonstrations in October 2008, together with the corresponding simulation results.

 
TU6PFP095 Beamline for Warm Dense Matter Experiment Using the KEK Digital Accelerator target, ion, heavy-ion, synchrotron 1519
 
  • T. Kikuchi, N. Harada, T. Sasaki
    Nagaoka University of Technology, Nagaoka, Niigata
  • C. Buttapeng, Namprom. Namprom
    University of the Thai Chamber of Commerce, Bangkok
  • K. Horioka
    TIT, Yokohama
  • K. Takayama
    KEK, Ibaraki
 
 

The KEK digital accelerator (KEKDA), which is an injector-free induction synchrotron capable of accelerating any ions with their possible charge state, is under construction*. This machine is an interesting device as a driver to explore a Warm Dense Matter (WDM) state. The irradiation onto a target at a small focal spot (< a few mm) with a short pulse duration (< 100 nsec) is required to create an interesting WDM state. The target temperature based on an equation-of-state fitted from SESAME table data is estimated as a function of the focal spot size and the ion number per bunch. Final focusing of an ion beam bunch extracted from KEKDA is realized through a half mini-beta system. For this purpose, the beamline has been carefully designed. Beam parameters, such as Twiss parameter, and the guiding magnet parameters will be given together with the drawing of the beamline.


*T. Adachi et al., “Modification of the KEK PS-Booster as a Digital Accelerator”, in this conference.

 
TU6PFP100 Temperature and Stress Rise Induced by Cracks in Accelerating Structures 1529
 
  • W. Zhu, T.M. Antonsen, J. Mizrahi, G.S. Nusinovich, G. Sharon
    UMD, College Park, Maryland
 
 

Funding: Office of High Energy Physics of DoE.


The achievable gradient of accelerating structures is limited by dark current capture, RF breakdown and cyclic fatigue. We consider only one effect related to the cyclic fatigue which can be important for reliable operation of high gradient structures, viz. the temperature and stress rise caused by the RF magnetic fields which can be increased in cracks. We made detailed analysis and simulations on the temperature and stress distribution and temporal evolution in the vicinity of cracks of different shapes on the copper when there is a heat flux, and compared the results to the case of a smooth metallic plane. We found out that the temperature will approximately double at the crack upper corners and stress will increase several times at the crack bottom at the beginning and then drop as the crack grows. This analysis gives some insight of the cyclic fatigue leading to the formation of microcracks and crack growth.

 
TU6RFP003 Commissioning of the New AGS MMPS Transformers power-supply, proton, controls, high-voltage 1538
 
  • E.M. Bajon, S.V. Badea, R. Bonati, I. Marneris, R. Porqueddu, T. Roser, J. Sandberg, S. Savatteri
    BNL, Upton, Long Island, New York
 
 

The Brookhaven AGS Main Magnet Power Supply is a thyristor control supply rated at 5.5KAmps, ±9KV. The peak magnet power is 50MW,which is fed from a motor/generator manufactured by Siemens. During rectify and invert operation, the P Bank power supplies are used. During the flattops the F Bank power supplies are used. The P Bank power supplies are fed from two 23MVA transformers and the F Bank power supplies are fed from two 5.3 MVA transformers. The fundamental frequency of the F Bank power supplies is 1440Hz while the P banks were 720Hz. It was very important to reduce the ripple during rectify to improve polarized proton operations. For this reason and also because the original transformers were 45 years old we replaced these transformers with new ones and we made the fundamental frequency of both P and F banks 1440 Hz. This paper will highlight the major hurdles that were involved during the installation of the new transformers. It will present waveforms while running at different power levels up to 6MW full load and show the transition from the F-Bank power supplies to the P-Banks and also show the improvements in ripple made on the P-Bank power supplies.

 
TU6RFP031 LHC Beam Dump System - Consequences of Abnormal Operation kicker, extraction, beam-losses, injection 1605
 
  • T. Kramer, B. Goddard, J.A. Uythoven
    CERN, Geneva
 
 

The LHC beam dump system is one of the most critical systems concerning machine protection and safe operation. It is used to dispose of high intensity beams between 450 GeV and 7 TeV. Studies into the consequences of abnormal beam dump actions have been performed. Different error scenarios have been evaluated using particle tracking in MAD-X, including an asynchronous dump action, and the impact of different orbit and collimator settings. Losses at locations in the ring and the beam dump transfer lines have been quantified as a function of different settings of the dump system protection elements. The implications for the setting up and operation of these protection elements are discussed.

 
TU6RFP033 AC Dipole System for Inter-Bunch Beam Extinction in the Mu2e Beam Line dipole, proton, electron, target 1611
 
  • E. Prebys, A.I. Drozhdin, C. Johnstone, N.V. Mokhov
    Fermilab, Batavia
  • C.M. Ankenbrandt
    Muons, Inc, Batavia
 
 

Funding: Supported under DOE contract DE-AC02-07CH11359.


The Mu2e experiment has been proposed at Fermilab to measure the rate for muons to convert to electrons in the field of an atomic nucleus with unprecedented precision. This experiment uses an 8 GeV primary proton beam consisting of short (~100 nsec) bunches, separated by 1.7 μs. It is vital that out-of-bunch beam be suppressed at the level of 10-9 or less. Part of the solution to this problem involves a pair of matched dipoles operating resonantly at half the bunch rate. There will be a collimation channel between them such that beam will only be transmitted when the fields are null. The magnets will be separated by 180 degrees of phase advance such that their effects cancel for all transmitted beam. Magnet optimization considerations will be discussed, as will optical design of the beam line. Simulations of the cleaning efficiency will also be presented.

 
TU6RFP046 Design and Diffractive Modeling on a Single Lens Shaper laser, alignment, radiation, gun 1650
 
  • C. Liu, S. Zhang
    JLAB, Newport News, Virginia
  • C. Liu
    PKU/IHIP, Beijing
 
 

Funding: DOE Contract DE-AC05-060R23177; China Scholarship Council


This paper introduces a single lens laser beam shaper which is capable of redistributing a beam with a Gaussian profile to a super-Gaussian profile. Both geometrical and diffractive optical modelings are performed on a typical single lens shaper that shows significant reduction of destructive effects on the beam uniformity over those with sharp-edges.

 
TU6RFP048 Upgrade of the FRIB Prototype Injector for Liquid Lithium Film Testing ion, electron, proton, gun 1656
 
  • S.A. Kondrashev, A. Barcikowski, Y. Momozaki, B. Mustapha, J.A. Nolen, P.N. Ostroumov, C.B. Reed, R.H. Scott
    ANL, Argonne
 
 

Funding: This work was supported by the U.S. Department of Energy, Office of Nuclear Physics, under Contract No. DE-AC02-06CH11357.


The development of a uniform and stable high velocity, thin liquid lithium film stripper is essential for the Facility for Rare-Isotope Beams (FRIB) Project. The formation of such a film has been demonstrated recently at ANL. Film thickness should be measured, and its temporal and spatial stability under high power ion beam irradiation should be verified. Intense beams of light ions generated by the FRIB prototype injector can be used for this task. The injector consists of an ECR ion source followed by a LEBT. A DC 3.3 mA/75 kV proton beam has been generated at the LEBT output. Proton beam power will be brought to required level by adding the second acceleration tube. A low energy electron beams (LEEB) technique, based on the thickness-dependent scattering of the electrons by the film, has been proposed as a fast-response on-line film thickness monitoring. A LEEB test bench has been built to verify this technique. The transmission of electrons through the carbon foils of different thicknesses was measured and compared with results of CASINO simulations. Agreement between the experimental and numerical results allows quantitative measurements of film thickness using the LEEB.

 
TU6RFP056 Design and Simulation of Microstrip Directional Coupler with Tight Structure and High Directivity target, coupling, impedance, cyclotron 1677
 
  • T. Hu, L. Cao, J. Huang, D. Li, B. Qin, J. Yang, T. Yu
    HUST, Wuhan
 
 

Funding: Nation Nature Science Foundation of China,10435030


The design study of Cyclotron CYCHU 10MeV has been developed at Huazhong University of Science and Technology (HUST). Because of the low center frequency (100MHz) of it’s RF system, we should choose suitable directional couplers for the RF system which is supposed to be high-directivity and tight-structure. This paper analyses and synthesizes kinds of directional couplers, espacially microstrip structure, for it’s tinier volume at the low center frequency compared with stripline and branch structures. The achievement of the high-directivity with microstrip configuration is carried out by the distributed capacitor to decrease the even and odd mode phase difference. Capacitive compensation is performed by the interdigital capacitors. The proposed structure is easy to fabricate and incorporate another microwave device due to planner microstrip.

 
TU6RFP064 Coaxial Coupler for X-Band Photocathode RF Gun gun, coupling, emittance, electron 1693
 
  • X.H. Liu, J.Q. Qiu, J. Shi, C.-X. Tang
    TUB, Beijing
 
 

Funding: This work is supported by National Natural Science Foundation of China(Project 10735050) and National Basic Research Program of China (973 Program)(Grant No. 2007CB815102).


The X-band photocathode RF gun can be utilized to generate electron beams with ultra-low emittance. In this paper, we present the design of a coaxial coupler for the X-band RF gun to avoid the emittance growth caused by field asymmetries. A detailed 3D simulation of the coupler is performed. The microwave circuit analysis is accomplished, and the relationship between the coupling factor and the coaxial coupler size is obtained. This paper likewise presents the beam dynamics parameters of the X-band RF gun with a coaxial coupler.

 
TU6RFP067 The Redesign, Installation of Light II-A Pulsed Power Generator and its Potential Application laser, pulsed-power, impedance, plasma 1702
 
  • C. Wang, X.D. Jiang, S.M. Wei, N.G. Zeng, T.J. Zhang
    CIAE, Beijing
  • J.Z. Wang
    Department of Physics, Central China Normal University, Wuhan
 
 

Light II-A pulsed power generator was used as a power driver of pumping KrF laser at CIAE. The redesign of Light II-A pulsed power generator is based on the consideration that the machine will consist of one single Marx generator with two different experimental lines,which is presented in this paper. The original experimental line with characteristic impedance of 5Ω is remained, and a new line of low impedance (about 1.5Ω ) is added to the Marx generator. The structure design and the electric insulation design are introduced. It is also outlined here the manipulation of modeling the dynamic behavior of gas discharge arc as well as the circuit simulation results of the two experimental lines. Meanwhile a brief introduction is given to the potential application of the low impedance line.

 
TU6RFP071 Development of a Prototype Bump Magnet for CSNS/RCS Injection injection, linac, synchrotron, target 1714
 
  • J.X. Song, Y. Hao, L.H. Huo, W. Kang, L. Wang
    IHEP Beijing, Beijing
 
 

China Spallation Neutron Source is a high intensity beam facility planed to build in future in China. It is composed of Linac, RCS and target station. Two sets of pulsed painting bump magnets, 4 magnets in each set , will be used in CSNS RCS to create a dynamic orbit bump for injection process. The design of these 8 bump magnets has been completed. One prototype bump magnet has been assembled and tested. In this paper, the magnetic field analysis, the eddy current and thermal consideration in the end plates of the prototype bump magnet are presented, and issues of the magnet development, construction and test are discussed.

 
TU6RFP073 Voltage Droop Compensation for High Power Marx Modulators klystron, impedance, high-voltage, controls 1717
 
  • D. Yu, P. Chen, M. Lundquist
    DULY Research Inc., Rancho Palos Verdes, California
 
 

Marx modulators, operated by the solid-state switches of Metal Oxide Semiconductor Field Effect Transistors (MOSFETs) or Insulated Gate Bipolar Transistors (IGBTs), offer an alternative to conventional high voltage modulators for rf power sources. They have the advantages of compact size, high-energy efficiency, high reliability, pulse width control and cost reduction. However, Marx modulators need a complex voltage compensation circuit if they are employed in long pulse applications such as the ILC project. We describe novel schemes to compensate the voltage droop of the Marx modulator and minimize the flattop fluctuation of the voltage pulse output through the utilization of inductances and the fast switching properties of solid-state switches. The feasibility of the schemes has been analyzed and relevant data will be presented.

 
TU6RFP076 Measurement of Longitudinal and Transverse Impedance of Kicker Magnets Using the Coaxial Wire Method impedance, kicker, resonance, coupling 1726
 
  • M.J. Barnes, F. Caspers, T. Kroyer, E. Métral, F. Roncarolo, B. Salvant
    CERN, Geneva
 
 

Fast kicker magnets are used to inject beam into and eject beam out of the CERN SPS accelerator ring. These kickers are generally ferrite loaded transmission line type magnets with a rectangular shaped aperture through which the beam passes. Unless special precautions are taken the impedance of the ferrite yoke can provoke significant beam induced heating, even above the Curie temperature of ferrite. In addition the impedance can contribute to beam instabilities. In this paper different variants of the coaxial wire method, both for measuring longitudinal and transverse impedance, are briefly discussed in a tutorial manner and do's and don'ts are shown on practical examples. In addition we present the results of several impedance measurements for SPS kickers using the wire method and compare those results with theoretical models.

 
TU6RFP077 Gap Clearing Kicker Magnet for Main Injector kicker, impedance, high-voltage, injection 1729
 
  • C.C. Jensen, R.E. Reilly, I. Terechkine
    Fermilab, Batavia
 
 

Funding: Fermilab is operated by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the United States Department of Energy.


A fast kicker magnet has been designed for use in Main Injector at Fermilab. The magnet will be used for controlled removal of unbunched beam created in the slip stacking process. The strength of each of the six magnets is 75 G·m at 500 A. The aperture is 11.4 cm wide x 5.3 cm high x 64 cm long. The field rise time from 3% to 97% of less than 57 ns has been achieved along with a flattop variation of less than ±3% variation. Results of simulation and measurements will be presented. The pulser is described in a companion paper.

 
TU6RFP082 Tests and Operational Experience with the DAΦNE Stripline Injection Kicker kicker, impedance, injection, damping 1739
 
  • F. Marcellini, D. Alesini, S. Guiducci, P. Raimondi
    INFN/LNF, Frascati (Roma)
 
 

New injection stripline kickers are operating since December 2007 at the DAΦNE collider. They are designed to operate with very short pulse generators to perturb only the injected bunch and the two stored adjacent ones at 2.7 ns and are a test for the design of the fast kickers of the damping ring of the International Linear Collider (ILC). Stripline frequency response and impedance measurements have been performed to characterize the structure and are compared to the simulation results. Operational performances are also described, pointing out the problems occured and the flexibility of the stripline structure that worked with both the short and the old pulse generators and has been used as an additional damping kicker to improve the efficiency of the horizontal multibunch feedback system.

 
TU6RFP088 Design of Electron Gun System for the PLS-II Linear Accelerator gun, electron, cathode, high-voltage 1751
 
  • Y.G. Son, K.R. Kim, S.H. Nam, S.J. Park
    PAL, Pohang, Kyungbuk
  • T. Asaka
    JASRI/SPring-8, Hyogo-ken
 
 

Funding: This work was supported by the MEST (Ministry of Education, Science and Technology) and the POSCO (POhang iron and Steel making COmpany) in Korea.


The PLS-II, the major upgrade program of the PLS (Pohang Light Source, a 2.5-GeV 3rd generation light source), is planned at the Pohang Accelerator Laboratory. The PLS 2.5-GeV linear accelerator, being the full-energy injector for the PLS storage ring, should be upgraded to provide the beam energy of 3 GeV. For the PLS-II linac, we are going to establish a dual electron gun system in which two guns will be on the accelerator beamline with a bending magnet enabling immediate switching of guns. The dual gun system is expected to achieve high reliability for the top-up injection to the PLS-II storage ring. Also the gun will be upgraded to provide the beam energy of 200 keV and a pulse high-voltage modulator will be constructed. Fifteen-section PFNs will be connected in series to make final impedance of approximately 17.3 ohm. A new modulator applying the inverter technology will be used to charge the PFN and obtain more stable charging performances. In this article the authours would like to report on the design status of the accelerator beamline and inverter modulator for the dual gun system.

 
WE1RAI03 Designing and Running for High Accelerator Availability power-supply, controls, monitoring, luminosity 1790
 
  • F.J. Willeke
    BNL, Upton, Long Island, New York
 
 

Overview of the main factors determining machine availability. Comparison of availability issues and strategy for high energy colliders and accelerators, synchrotron light sources, and spallation neutron sources. Description of how machines can be designed for high availability and systems for high reliability.

 

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WE1PBI03 Cyclotron Resonances in Electron Cloud Dynamics electron, resonance, cyclotron, wiggler 1807
 
  • C.M. Celata, M.A. Furman, J.-L. Vay
    LBNL, Berkeley, California
  • D.P. Grote
    LLNL, Livermore, California
  • J.S.T. Ng, M.T.F. Pivi, L. Wang
    SLAC, Menlo Park, California
 
 

Funding: This work was supported by the Office of Science, U. S. Department of Energy, under Contract No. DE-AC02-05CH11231.


A new set of resonances for electron cloud dynamics in the presence of a magnetic field has been found. For short beam bunch lengths and low magnetic fields where lb << 2*π/ωc, (lb = bunch duration, ωc = non-relativistic cyclotron frequency) resonances between the bunch frequency and harmonics of the cyclotron frequency cause an increase in the electron cloud density in narrow ranges of magnetic field near the resonances. For ILC parameters the increase in the density is up to a factor of approximately 3, and the spatial distribution of the electrons is broader near resonances, lacking the well-defined density "stripes" of multipactoring found for non-resonant cases. Simulations with the 2D computer code POSINST, as well as a single-particle tracking code, were used to elucidate the physics of the dynamics. The resonances are expected to affect the electron cloud dynamics in the fringe fields of conventional lattice magnets and in wigglers, where the magnetic fields are low. Results of the simulations, the reason for the bunch-length dependence, and details of the dynamics will be discussed.


C.M. Celata is presently also a visitor in Physics, Mathematics, and Astronomy at California Institute of Technology.

 

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WE1PBC04 The New RF Deflectors for the CTF3 Combiner Ring damping, electron, multipactoring, cavity 1812
 
  • D. Alesini, A. Ghigo, F. Marcellini
    INFN/LNF, Frascati (Roma)
  • J.F. DeFord
    STAAR/AWR Corporation, Mequon
  • V.A. Dolgashev
    SLAC, Menlo Park, California
  • G. McMonagle
    CERN, Geneva
 
 

To suppress the vertical beam instability in the CTF3 Combiner Ring caused by vertical trapped modes in the rf deflectors, two new devices have been constructed. In the new structures special antennas absorb the power released by the beam to the modes. They have been realized in aluminium to reduce the costs and delivery time and have been successfully installed in the ring. In the paper we illustrate the electromagnetic design, the realization procedures, the rf measurement and high power test results.

 

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WE1GRC05 Crystal Collimation Studies at the Tevatron (T-980) collimation, beam-losses, collider, target 1836
 
  • N.V. Mokhov, G. Annala, A. Apyan, R.A. Carrigan, A.I. Drozhdin, T.R. Johnson, A.M. Legan, R.E. Reilly, V.D. Shiltsev, D.A. Still, R. Tesarek, J.R. Zagel
    Fermilab, Batavia
  • R.W. Assmann, V.P. Previtali, S. Redaelli, W. Scandale
    CERN, Geneva
  • Y.A. Chesnokov, I.A. Yazynin
    IHEP Protvino, Protvino, Moscow Region
  • V. Guidi
    INFN-Ferrara, Ferrara
  • Yu.M. Ivanov
    PNPI, Gatchina, Leningrad District
  • S. Peggs
    BNL, Upton, Long Island, New York
  • M. Prest
    Università dell'Insubria & INFN Milano Bicocca, Como
  • S. Shiraishi
    Enrico Fermi Institute, University of Chicago, Chicago, Illinois
 
 

Funding: Work supported by Fermi Research Alliance, LLC, under contract No. DE-AC02-07CH11359 with the U.S. Department of Energy.


Bent-crystal channeling is a technique with a potential to increase the beam-halo collimation efficiency at high-energy colliders. First measurements at the Tevatron in 2005 have shown that using a 5-mm silicon crystal to deflect the proton beam halo onto a secondary collimator improves the system performance by reducing the machine impedance, beam losses in the collider detectors and irradiation of the superconducting magnets, all in agreement with simulations. Recent results, obtained with substantially improved goniometer and enhanced beam diagnostics, are reported showing channeling collimation of the ~1-TeV circulating proton beam halo at the Tevatron collider. Comprehensive results of computer modeling are presented which allow further developments of the T-980 experiment towards a robust system compatible with requirements to high-efficient collimation at the Tevatron and LHC hadron colliders.

 

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WE2PBC04 Coupler Kicks in the Third Harmonic Module for the XFEL cavity, wakefield, HOM, acceleration 1858
 
  • E. Gjonaj, W. Ackermann, T. Lau, T. Weiland
    TEMF, TU Darmstadt, Darmstadt
  • M. Dohlus
    DESY, Hamburg
 
 

The rf and wakefield transverse kicks resulting from the asymmetry of input and HOM couplers in the third harmonic module for the XFEL are investigated. The fundamental mode is computed using eigenvalue analysis. The short range wakefields in a string of cavities are simulated with the PBCI code. Using the simulation data, the transverse kick factors associated with the presence of cavity couplers are evaluated.


* P. Pierini, "Third Harmonic Superconducting Cavity Prototypes for the XFEL", LINAC08.
** T. Khabiboulline, "New HOM Coupler Design For 3.9 Ghz Superconducting Cavities At FNAL", PAC07.

 

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WE3RAC06 Development of the Model of a Self Excited Loop feedback, controls, cavity, linac 1886
 
  • G. Joshi
    BARC, Trombay, Mumbai
  • V. Agarwal, G. Kumar
    Indian Institute of Technology Bombay, Mumbai
  • R.G. Pillay
    TIFR, Mumbai
 
 

As a first step towards development in digital domain, a computer model of a self excited loop (SEL) has been created using MATLAB/SIMULINK. The behaviour of a resonator and a power amplifier combination has been approximated using two first-order differential equations. The square of the amplitude of the RF field in the resonator acts as a driving force for the motion of mechanical modes of the resonator, which are individually represented as second order systems. A key element is the limiter, which has been modelled as a feedback loop, to achieve constant output amplitude. The model has been created in the I-Q domain for computational efficiency and close correspondence with actual implementation. To study the field stabilisation, proportional amplitude and phase feedback loops have been appended to the model of the SEL. In this paper we discuss the details of the model and results from simulation. Initial experimental results are also presented.

 

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WE3PBI03 LHC Beam-Beam Compensation Studies at RHIC electron, proton, beam-beam-effects, collider 1899
 
  • W. Fischer, R. Calaga, R. De Maria, Y. Luo, N. Milas, C. Montag, G. Robert-Demolaize
    BNL, Upton, Long Island, New York
  • H.J. Kim, T. Sen
    Fermilab, Batavia
 
 

Funding: Work supported by U.S. DOE under contract No DE-AC02-98CH1-886


Long-range and head-on beam-beam effects are expected to limit the LHC performance with design parameters. To mitigate long-range effects current carrying wires parallel to the beam were proposed. Two such wires are installed in RHIC where they allow studying the effect of strong long-range beam-beam effects, as well as the compensation of a single long-range interaction. The tests provide benchmark data for simulations and analytical treatments. To reduce the head-on beam-beam effect electron lenses were proposed for both the LHC and RHIC. We present the experimental long-range beam-beam program and report on head-on compensations studies at RHIC, which are primarily based on simulations.

 

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WE3PBC05 Advanced Simulation and Optimization Tools for Dynamic Aperture of Non-Scaling FFAGs and Related Accelerators Including Modern User Interfaces lattice, dynamic-aperture, proton, cyclotron 1907
 
  • C. Johnstone, V. Kashikhin
    Fermilab, Batavia
  • M. Berz, K. Makino
    MSU, East Lansing, Michigan
  • P. Snopok
    St. Petersburg State University, St. Petersburg
 
 

Innovations in computer techniques in combination with increased sophistication in modeling are required to accurately understand, design and predict high-energy, and, in particular, the new generation of frontier accelerators for HEP and other applications. A recently identified problem lies in the simulation and optimization of FFAGs and related devices, for which currently available tools provide only approximate and inefficient simulation. For this purpose new tools are being developed within the advanced accelerator code COSY INFINITY to address complex, specific electromagnetic fields, including high-order fringe fields, out of plane fields, edge effects, and general field profiles; tools linked to modern global optimization techniques that can further accommodate the ultra-large emittances of proposed beams to allow efficient probing of very high dimensional parameter space. This new set of tools based on modern techniques and simulation approaches will be furnished with modern GUI-based user interfaces.

 

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WE4PBC03 A High-Duty Factor Radio-Frequency Quadrupole Accelerator for ADS Study in China rfq, controls, LLRF, coupling 1955
 
  • H.F. Ouyang, S. Fu, K.Y. Gong, T. Huang, J. Li, J.M. Qiao, T.G. Xu, X.A. Xu, Y. Yao, H.S. Zhang, Z.H. Zhang, F.X. Zhao
    IHEP Beijing, Beijing
  • J.X. Fang, Z.Y. Guo
    PKU/IHIP, Beijing
  • X. Guan
    CIAE, Beijing
 
 

A high-duty factor proton RFQ accelerator has been constructed at IHEP, Beijing for the basic study of Accelerator Driven Subcritical System. The ADS basic study is supported by a national program for nuclear waste transmutation which is regarded essential for the rapid development of nuclear power plants in China. In the initial commissioning of the 3.5MeV RFQ with an ECR ion source showed a nice performance with a transmission rate about 93% with an output beam of 46mA. The 352MHz RFQ is design for CW operation with the RF power source from LEP-II of CERN. This paper presents the beam commissioning and recent progress in high-duty factor operation from 7% to 15%.

 

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WE4GRC02 Measurement of Electron Cloud Development in the Fermilab Main Injector Using Microwave Transmission electron, pick-up, coupling, quadrupole 1967
 
  • N. Eddy, J.L. Crisp, I. Kourbanis, K. Seiya, R.M. Zwaska
    Fermilab, Batavia
  • S. De Santis
    LBNL, Berkeley, California
 
 

The production of an Electron Cloud poses stability issues for future high intensity running of the Fermilab Main Injector. Recent experiements have shown the presense of the electron cloud can be detected by the phase shift of a TE wave propagated along the beampipe. This technique has been employed to provide very sensitive measurements of the electron cloud development in the Fermilab Main Injector.

 

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WE5PFP001 The Effects of Field Emitted Electrons on RF Surface electron, cavity, site, controls 1982
 
  • A. Zarrebini, M. Ristic
    Imperial College of Science and Technology, London
  • A. Kurup, K.R. Long, J.K. Pozimski
    Imperial College of Science and Technology, Department of Physics, London
  • R. Seviour, M.A. Stables
    Cockcroft Institute, Lancaster University, Lancaster
 
 

The proposed Muon Cooling System for the Neutrino Factory operates with high accelerating gradient in the presence of magnetic field. This can significantly increase the risk of RF breakdown. Field Emission is the most frequently encountered RF breakdown that occurs at sites with local electromagnetic field enhancement. Surface defects can be considered as possible emission sites. Upon Impact, generally the majority of electron’s energy is converted into stress and heat. In return, the damage inflicted can create additional emission sites. This paper presents the work under way, which aims to model certain physical phenomena during both emission and impact of electrons. The three-dimensional field profile of an 805 MHz pill-box cavity is modelled by Comsol Multuphysics. A tracking code written in-house is employed to track particles, providing sufficient data such as energy and speed at small time steps. This would allow the study of local heat transfer, applied surface stresses and secondary electron yield upon impact with the RF surface. In addition, the effects of externally applied magnetic field on electron’s behaviour are to be investigated.

 
WE5PFP007 Building Twisted Waveguide Accelerating Structures acceleration, cavity, electron, controls 1997
 
  • M.H. Awida
    University of Tennessee, Knoxville, Tennessee
  • M.H. Awida
    ORNL RAD, Oak Ridge, Tennessee
  • Y.W. Kang, S.-H. Kim, S.W. Lee, J.L. Wilson
    ORNL, Oak Ridge, Tennessee
 
 

RF properties of twisted waveguide structures were investigated to show that slow-wave accelerating fields can be excited and used for acceleration of particle at various velocities lately. To build a practical accelerating cavity structure using the twisted waveguide, more development work was needed: cavity structure tuning, end wall effect of the structures, incorporating beam pipes and input power coupler, and HOM damping, etc. In this paper, the practical aspects of the designs to make more complete accelerating structures are discussed with the results of computer simulations.

 
WE5PFP009 RF Breakdown Studies Using a 1.3-GHz Test Cell cavity, vacuum, pick-up, electron 2003
 
  • M. BastaniNejad, A.A. Elmustafa
    Old Dominion University, Norfolk, Virginia
  • J.M. Byrd, D. Li
    LBNL, Berkeley, California
  • M.E. Conde, W. Gai
    ANL, Argonne
  • R.P. Johnson, M.L. Neubauer, R. Sah
    Muons, Inc, Batavia
  • A. Moretti, M. Popovic, K. Yonehara
    Fermilab, Batavia
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-08ER86352 and FRA DOE contract number DE-AC02-07CH11359


Many present and future particle accelerators are limited by the maximum electric gradient and peak surface fields that can be realized in RF cavities. Despite considerable effort, a comprehensive theory of RF breakdown has not been achieved and mitigation techniques to improve practical maximum accelerating gradients have had only limited success. Recent studies have shown that high gradients can be achieved quickly in 805 MHz RF cavities pressurized with dense hydrogen gas without the need for long conditioning times, because the dense gas can dramatically reduce dark currents and multipacting. In this project we use this high pressure technique to suppress effects of residual vacuum and geometry found in evacuated cavities to isolate and study the role of the metallic surfaces in RF cavity breakdown as a function of magnetic field, frequency, and surface preparation. A 1.3-GHz RF test cell with replaceable electrodes (e.g. Mo, Cu, Be, W, and Nb) and pressure barrier capable of operating both at high pressure and in vacuum been designed and built, and preliminary testing has been completed. A series of detailed experiments is planned at the Argonne Wakefield Accelerator.

 
WE5PFP012 RF Deflector for Bunch Length Measurement at Low Energy at PSI cavity, emittance, gun, FEL 2012
 
  • A. Falone, H. Fitze, R. Ischebeck, Y. Kim, M. Pedrozzi, V. Schlott, B. Steffen, L. Stingelin
    PSI, Villigen
  • D. Alesini, L. Ficcadenti, L. Palumbo
    INFN/LNF, Frascati (Roma)
 
 

RF deflectors are crucial diagnostic tools for bunch length and slice emittance measurements with sub-picosecond resolution. Their use is essential in commissioning and operation of VUV and X-ray FELs. The 250MeV FEL injector, under construction at PSI, will use two of them. The first one will be installed after the gun at low energy (~7MeV), the second one at the end of the Linac at high energy (250MeV). The first RF deflector consists of a single cell standing wave cavity working on the TM110 deflecting mode, and tuned at 2997.912 MHz (frequency of the linac structures). In this note we report the motivation of this measurement, beam dynamics and beam diagnostics considerations and the RF design and simulations of this cavity.

 
WE5PFP020 Multipacting Simulation for Muon Collider Cavity cavity, collider, electron, monitoring 2033
 
  • L. Ge, K. Ko, Z. Li, C.-K. Ng
    SLAC, Menlo Park, California
  • D. Li
    LBNL, Berkeley, California
  • R. B. Palmer
    BNL, Upton, Long Island, New York
 
 

Funding: This work was supported by DOE contract No. DE-AC02-76SF00515 NERSC


The muon cooling cavity for Muon Collider works under strong external magnetic fields. It has been observed that this external magnetic field can enhance the multipacting activities and dark current heating. As part of a broad effort to optimize external magnetic field map and cavity shape for minimal dark current and multipacting, we use SLAC’s 3D parallel code Track3P to analyze the multipacting and dark current issues of the design. Track3P has been successfully used to predict multipacting phenomena in cavity and coupler designs. It provides unprecedented capabilities for simulating large-scale accelerator structure systems, including realistic 3D details and low turn-around times. In this paper, we present the comprehensive multipacting and dark current simulations for Muon Collider cavities.

 
WE5PFP023 The Backward TW Structure for the FERMI@Elettra Linac coupling, cavity, linac, klystron 2042
 
  • C. Serpico, P. Craievich, C. Pasotti
    ELETTRA, Basovizza
 
 

Funding: The work was supported in part by the Italian Ministry of University and Research under grant FIRB-RBAP045JF2 or grant FIRB-RBAP06AWK3 or grants FIRB-RBAP045JF2 and FIRB-RBAP06AWK3


The FERMI@ELETTRA project will use the existing ELETTRA linac. The linac includes seven accelerating sections, each section is a backward traveling (BTW) structure comprised of 162 nose re-entrant cavities coupled magnetically. Furthermore, there are specialized input and output cavities specifically designed to match the structure to the RF source and load. These BTW accelerating structures work on the 3pi/4 mode which was chosen to optimize the structure efficiency and to achieve a simple RF tuning setup. These accelerating sections are powered by a TH2132A 45 MW klystron providing a 4.5 microsecond rf pulse and are coupled to a Thomson CIDR. In this paper the 3pi/4 backward BTW structures are investigated and the results of the electromagnetic simulations are presented.

 
WE5PFP025 Numerical Calculus of Resonant Frequency Change by 3D Reconstruction of Thermal Deformed Accelerator Tube cavity, electron, linac, resonance 2048
 
  • Z. Shu, M.J. Li, L.G. Shen, Y. Sun, X.C. Wang, W. Zhao
    USTC/PMPI, Hefei, Anhui
  • Y.J. Pei
    USTC/NSRL, Hefei, Anhui
 
 

Funding: "Collinear Load for Accelerators and R&D on High Power Microwave Absorbed Material" No.10775128 From National Natural Science Foundation of China


Thermal deformation caused by Non-uniform temperature distribution in disk-loaded waveguide will affect the resonant frequency of LINAC deeply. Formerly, researchers evaluated it by experiments or experience and gave their conclusion roughly and linearly. A new approach of integration of multi-disciplinary is adopted to study the relationship more accurately. After loading the loss RF power on the accelerator tube wall, the thermal deformation is calculated in software I-DEAS, and a deformed finite element model is obtained. Then nodes on inner surfaces of the cavities were extracted and sort by a customized program. According to these nodes, a new solid model is reconstructed with a self developed 3D reconstruction technology in ANSYS. B-Spline interpolation technique is used to fit a group of curves first, and then to reconstruct NURBS surfaces. The final reconstructed deformed solid model, obtained by closing the surfaces, can be exported in IGES format which is used to recalculate the resonant frequency in Microwave Studio again. The error of the reconstruction can be controlled within 3 micrometers. The resonant frequency change of every cavity can be accurately calculated.


Parietti L, etc., Thermal structural analysis and frequency shift **
Zhou, Zu-Sheng,etc. Thermal structural analysis and test **

 
WE5PFP028 Using Cerenkov Light to Detect Field Emission in Superconducting Cavities cavity, electron, diagnostics, photon 2052
 
  • Y. Torun
    IIT, Chicago, Illinois
 
 

Superconducting RF cavities are made of a thin metal shell (typically Niobium) with liquid Helium around it housed within another metal vessel. This geometry is effectively a Cerenkov radiator between two mirrors. Electrons stripped from the inner surface due to field emission can get accelerated by the electric field inside the cavity, punch through the cavity wall and still have enough energy to be faster than light in He. Detection of Cerenkov light generated by the electrons through an optical port integrated into the vessel can serve as a very sensitive diagnostic for field emission in cavity R&D and production as well as in operating superconducting linear accelerators. We report on simulation results for calculating the effective light yield in such a system to establish the feasibility of the technique.

 
WE5PFP029 RF Power Coupler Developments for Superconducting Spoke Cavities at IPN Orsay vacuum, cavity, electron, rf-amplifier 2055
 
  • E. Rampnoux, S. Berthelot, P. Blache, S. Bousson, J. Lesrel, L. Lukovac, G. Olry
    IPN, Orsay
 
 

Funding: EURISOL Project


The development of RF power couplers for superconducting low-beta SPOKE cavities, performed at Nuclear Physics Institute in Orsay in the framework of the EURISOL Design Study, has led to the design of a 20 kW RF power coaxial coupler showing very good RF performances and the implementation of a test stand to condition two of these couplers at 20 kW CW power in the traveling wave mode at 352,2 MHz by using a half-wave resonant cavity. Composed by a ceramic disk, the coaxial power coupler developed shows on one hand a very good 50 ohms matching on a large bandwidth like 760 MHz, after an electromagnetic optimisation of the window area, and on the other hand a simplified design with regard to the classic coaxial couplers. Characteristics of the power coupler and the test stand will be described, and the low RF power test of the coaxial window and the conditioning at high RF power of two couplers will be presented.

 
WE5PFP032 Cold Testing and Recent Results of the Blade Tuner for CM2 at FNAL cavity, cryomodule, insertion, linac 2061
 
  • R. Paparella, A. Bosotti, C. Pagani, N. Panzeri
    INFN/LASA, Segrate (MI)
  • J. Knobloch, O. Kugeler, A. Neumann
    BESSY GmbH, Berlin
 
 

An extensive validation activity has been conducted since year 2007 for the coaxial Blade Tuner for TESLA SC cavities. During this activity, performances and limits of prototype models have been deeply investigated through detailed test sessions inside CHECHIA (DESY) and HoBiCaT (BESSY) horizontal cryostats as well as F.E. modeling and analyses. The result is an improved design for the Blade Tuner, specifically meant to satisfy the incoming ILC-level performance requirements, fulfill pressure vessels regulations and keep Ti / S.S. material compatibility. Recent Blade Tuner activities and results will be presented in this paper in view of the installation of 8 units in the second cryomodule of ILCTA facility at Fermilab, and also of our contribution to both incoming S1-Global (KEK) and ILC-HiGrade projects. The manufacturing process of the first set of 8 tuners, from production to room temperature validation for the whole series, will be also reviewed. Then results will be shown from the cold tests recently performed, where special effort has been made in evaluating the accuracy and repeatability of fast and slow tuning action at few Hz range.

 
WE5PFP046 Dark Current Simulation for the CLIC T18 High Gradient Structure electron, cavity, collider, linear-collider 2101
 
  • Z. Li, A.E. Candel, L. Ge, K. Ko, C.-K. Ng, G.L. Schussman
    SLAC, Menlo Park, California
  • S. Döbert, M. Gerbaux, A. Grudiev, W. Wuensch
    CERN, Geneva
  • T. Higo, S. Matsumoto, K. Yokoyama
    KEK, Ibaraki
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


Normal conducting accelerator structures such as the X-Band NLC structures and the CLIC structures have been found to suffer damage due to RF breakdown and/or dark current when processed to high gradients. Improved understanding of these issues is desirable for the development of structure designs and processing techniques that improve the structure high gradient performance. While vigorous experimental efforts have been put forward to explore the gradient parameter space via high power testing, comprehensive numerical multipacting and dark current simulations would complement measurements by providing an effective probe for observing interior quantities. In this paper, we present studies of multipacting, dark current, and the associated surface heating in high gradient accelerator structures using the parallel finite element simulation code Track3P. Comparisons with the high power test of the CLIC accelerator structures will be presented.

 
WE5PFP047 A Compact Alternative Crab Cavity Design at 400-MHz for the LHC Upgrade cavity, HOM, damping, electron 2104
 
  • Z. Li, L. Xiao
    SLAC, Menlo Park, California
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


Crab cavities are proposed for the LHC upgrade to improve the luminosity. In the local crabbing scheme, the crab cavities are located close to the interaction region and the transverse separation between the two beam lines at the crab cavity location can only accommodate an 800-MHz cavity of the conventional elliptical shape. Thus the baseline crab cavity design for the LHC upgrade is focused on the 800-MHz elliptical cavity shape although a lower frequency cavity is preferable due to the long bunch length. In this paper, we present a compact 400-MHz design as an alternative to the 800-MHz baseline design. The compact design is of a half-wave resonator (HWR) shape that has a small transverse dimension and can fit into the available space in the local crabbing scheme. The optimization of the HWR cavity shape and the couplers for the HOM, LOM, and SOM damping will be presented.

 
WE5PFP048 800MHz Crab Cavity Conceptual Design for the LHC Upgrade cavity, HOM, coupling, damping 2107
 
  • L. Xiao, Z. Li, C.-K. Ng, A. Seryi
    SLAC, Menlo Park, California
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


In this paper, we present a 800MHz crab cavity conceptual design for LHC upgrade, including the cell shape optimization, and LOM, SOM, HOM and input coupler design. The compact coax-to-coax coupler scheme is proposed to couple to the LOM and SOM modes which can provide strong coupling to the LOM and SOM modes. HOM coupler design uses a two-stub antenna with a notch filter to couple to the HOM modes in the horizontal plane and reject the operating mode at 800MHz. All the damping results for the LOM/SOM/HOM modes satisfy their damping requirements. The multipacting in cell and couplers is simulated as well. And the issue of the cross-coupling between the input coupler and LOM/SOM couplers due to cavity asymmetry is addressed. The power coming out of the LOM/SOM/HOM couplers are estimated. All the simulations are carried out using SLAC developed parallel EM simulation codes Omega3P, S3P and Track3P.

 
WE5PFP053 Design of Superconducting Parallel Bar Deflecting and Crabbing RF Structures cavity, HOM, damping, RF-structure 2120
 
  • J.R. Delayen, H. Wang
    JLAB, Newport News, Virginia
  • J.R. Delayen
    ODU, Norfolk, Virginia
 
 

Funding: Authored by Jefferson Science Associates, LLC under U.S. DOE Contract No. DE-AC05-06OR23177


A new concept for a deflecting and crabbing rf structure based on half-wave resonant lines was introduced recently*. It offers significant advantages to existing designs and, because of it compactness, allows low frequency operation. This concept has been further refined and optimized for superconducting implementation. Results of this optimization and application to a 400 MHz crabbing cavity and a 499 MHz deflecting cavity are presented.


*A New TEM-Type Deflecting and Crabbing RF Structure, J. R. Delayen and H. Wang, Proc. LINAC08

 
WE5PFP059 Design, Prototype and Measurement of a Single-Cell Deflecting Cavity for the Advanced Photon Source cavity, damping, impedance, cryomodule 2138
 
  • H. Wang, G. Cheng, G. Ciovati, P. Kneisel, R.A. Rimmer, K. Tian, L. Turlington
    JLAB, Newport News, Virginia
  • R. Nassiri, G.J. Waldschmidt
    ANL, Argonne
 
 

Funding: This manuscript has been authored by Jefferson Science Associates, LLC and by UChicago Argonne, LLC under U.S. DOE Contract numbers DE-AC05-06OR23177 and DE-AC02-06CH11357.


After design optimization of a squashed elliptical single-cell crab cavity at 2.8 GHz, a copper prototype has been bench measured in order to determine its rf properties and the effectiveness of waveguide damping of parasitic modes, especially the low-order mode (LOM)*. We also present detailed results of the RF cold test at 2K on niobium single-cell and two-cell prototype cavities operating either in the zero or pi mode. Further progress will be discussed on the design of high-order mode (HOM) waveguide damping, the analysis of the Lorenz force detuning simulations by ANSYS, and the prototype of on-cell damping in which a waveguide port is attached directly on the cavity’s long equator. Details of LOM/HOM impedance calculations and experimental bench measurements will be reported and compared to strict requirements for satisfying the APS impedance budget.


*J. Shi et. al., “Superconducting RF Deflecting Cavity Design and Prototype for Short X-ray Pulse Generation”, EPAC 2008, paper MOPP155.

 
WE5PFP061 Commissioning of the SRF Surface Impedance Characterization System at Jefferson Lab cavity, impedance, SRF, niobium 2144
 
  • B. Xiao, R.L. Geng, F. Marhauser, H.L. Phillips, C.E. Reece, H. Wang
    JLAB, Newport News, Virginia
  • M.J. Kelley
    The College of William and Mary, Williamsburg
 
 

Funding: Authored by Jefferson Science Associates, LLC under U.S. DOE Contract No. DE-AC05-06OR23177.


Much remains to be learned regarding the details of SRF performance effects with material variation, including niobium treated in different ways, and different bulk/thin film materials that are fabricated under different conditions. A facility that can measure small samples’ RF properties in a range of 0~180mT magnetic field and 2~20k temperature is necessary in order to answer this question. The Jefferson Lab surface impedance characterization (SIC) system has been designed to attempt to meet this requirement. The SIC system uses a sapphire-loaded cylindrical Nb cavity at 7.5GHz with 50mm diameter flat sample placed on a non-contacting end plate and a calorimetric technique to directly measure the rf dissipation in the sample in response to known rf fields over ~1 cm2. We report on the commissioning of this system and its first uses for characterizing materials. Preliminary tests with Nb thin film sample sputtered on Cu substrate, and bulk Nb sample have been done at low field. The presently available hardware is expected to enable tests up to 20 mT peak magnetic field on the sample CW. Paths to higher field tests have been identified.

 
WE5PFP068 Linear-Quadratic-Gaussian Controllers for Single-Frequency RF Systems and Short Bunches in NSLS-II feedback, controls, cavity, klystron 2162
 
  • N.A. Towne, H. Ma, J. Rose
    BNL, Upton, Long Island, New York
 
 

Funding: Work performed under contract number 126615 for Brookhaven Science Associates, LLC.


NSLS-II is a new ultra-bright 3GeV 3rd generation synchrotron radiation light source. The performance goals require operation with a beam current of 500mA and a bunch current of at least 0.5mA. The position and timing specifications of the photon beam place tolerances on the phase stability of the RF cavity fields of less than 0.15 degrees jitter. This study develops computational methods for the construction of LQG controllers for discrete-time models of single-cavity rf systems coupled to rigid-bunch beams able to meet this tolerance. It uses Matlab’s control-systems toolbox and Simulink to synthesize the LQG controller; establish resolutions of state variables, ADCs, DACs, and matrix coefficients that, in a fixed-point controller provide essentially undiminished performance; simulate closed-loop performance; and assess sensitivity to variations of the model. This machinery is applied to NSLS-II-, CLS-, and NSLS VUV-ring models showing exceptional noise suppression and bandwidth. Thoughts are given on the validation and tuning of the rf model by machine measurements, DSP implementations, and future work.

 
WE5PFP070 Modelling and Simulation of the RF System for SPIRAL2 cavity, feedback, controls, linac 2168
 
  • O. Piquet, M. Luong
    CEA, Gif-sur-Yvette
 
 

The acceleration of non relativistic particles, with a velocity lower than light velocity, in an RF cavity is more complex than for relativistic particles. Non-linear behaviours appear on the accelerator voltage because of the phase slippage inside the cavity. Moreover, a superconducting RF cavity is sensitive to various perturbations like mechanical vibrations (microphonics) and Lorentz force detuning. These perturbations produce a significant detuning of the cavity, leading a strong instability for the amplitude and phase of the field because of the narrow bandwidth of the accelerating mode. We will present a simulation approach of the cavity and its LLRF system control in order to ensure proper cavity operation under perturbations in the framework of the SPIRAL2 project.

 
WE5PFP071 Transient Analysis of RF Cavities under Beam Loading cavity, impedance, coupling, LLRF 2171
 
  • H. Hassanzadegan, R. Grino
    UPC, Barcelona
  • D. Einfeld
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The conventional electrical model analogy of a RF cavity is a shunt RLC circuit supplied by two current sources representing the RF amplifier and the beam. In the literature, the impedance of the cavity is often calculated in the Fourier domain. This type of cavity modelling has two drawbacks: First, it assumes a perfect matching between the cavity and the amplifier therefore it neglects the reflected voltage. And, second, it does not provide any information about the cavity transient response, for example at startup or upon beam arrival, while this information can be very important for the design of the regulation loops. In this work we will remove these drawbacks by calculating the cavity impedance in Laplace domain taking the reflected voltage into account. We will then modify our model so that it also includes the influence of the beam on the cavity. For transient RF simulations, though, a typical problem is the long simulation time due to the relatively slow transient response compared to the RF period. To overcome this problem, finally, we will use a mathematical method to map the cavity frequency response from RF to baseband to reduce the simulation time significantly.

 
WE5PFP095 Application of Non-Linear Time-Domain RF Simulations to Longitudinal Emittance Studies for the LHC LLRF, emittance, feedback, klystron 2234
 
  • T. Mastorides, J.D. Fox, C.H. Rivetta, D. Van Winkle
    SLAC, Menlo Park, California
 
 

Funding: Work supported by the U.S. Department of Energy under contract # DE-AC02-76SF00515 and the US-LARP program


A non-linear time-domain simulation has been developed that can determine technical limitations, effects of non-linearities and imperfections, and impact of additive noise on the interaction of the beam with the Impedance Control Radio Frequency (RF) systems [1]. We present a formalism for the extraction of parameters from the time-domain simulation to determine the sensitivity of the beam longitudinal emittance and dilution on the RF system characteristics. Previous studies [2], [3] have estimated the effect of a noise source on the beam characteristics assuming an independent perturbation source of the RF voltage and a simplified beam model with no coupling. We present the methodology for the time-domain simulation study of the dependence of the accelerating voltage noise spectrum on the various RF parameters and the technical properties (such as non-linearities, thermal noise, frequency response etc.) of the Low Level RF (LLRF) system components. Future plans to expand this formalism to coupled bunch studies of longitudinal emittance growth in the LHC at nominal and upgraded beam currents are briefly summarized.

 
WE5PFP100 Beam Loading Effects on the RF Control Loops of a Double-Harmonic Cavity System for FAIR cavity, controls, beam-loading, resonance 2249
 
  • D. Lens
    TU Darmstadt, RTR, Darmstadt
  • P. Hülsmann, H. Klingbeil
    GSI, Darmstadt
 
 

Funding: This work was partly supported by Deutsche Telekom Stiftung.


The effects of heavy beam loading on the RF control loops of a double-harmonic cavity system are examined. This cavity system that will be realized at the GSI Helmholtzzentrum für Schwerionenforschung in the scope of the SIS18 upgrade program consists of a main broadband cavity and a second harmonic narrowband cavity. The cavities comprise both an amplitude and a phase feedback loop. In addition, the narrowband cavity includes a feedback loop which controls its resonance frequency to follow the main RF frequency. After modelling the cavity system and the feedback loops, an analytic controller design is presented. In addition, longitudinal beam dynamics are added to the cavity model to allow a detailed simulation of the cavity-beam interaction. Realistic simulation results are given for an acceleration cycle of heavy-ions to demonstrate the performance of the RF control loops.

 
WE5PFP101 RF System Modeling for the CEBAF Energy Upgrade cavity, controls, LLRF, superconducting-cavity 2252
 
  • T. E. Plawski, C. Hovater
    JLAB, Newport News, Virginia
 
 

Funding: Notice: Authored by Jefferson Science Associates, LLC under U.S. DOE Contract No. DE-AC05-06OR23177.


The RF system model based on MATLB has been developed for analyzing the basic characteristics of the LLRF control system being designed for the 12 GeV Energy Upgrade of the CEBAF accelerator. In our model, a typically complex cavity representation is simplified to in-phase and quadrature (I&Q) components. Lorentz Force and microphonic detuning is incorporated as a new quadrature carrier frequency (frequency modulation). Beam is also represented as in-phase and quadrature components and superpositioned with the cavity field vector. Afterward signals pass through two low pass filters, where the cutoff frequency is equal to half of the cavity bandwidth then they are demodulated using the same detuning frequency. Because only baseband I&Q signals are calculated, the simulation process is very fast when compared to other controller-cavity models. During the design process we successfully analyzed gain requirements vs. field stability for different superconducting cavity microphonic backgrounds and Lorentz Force coefficients. Moreover, we were able to evaluate different types of a LLRF structures:GDR* and SEL** as well as klystron power requirements for different cavities and beam loads.


*Generator Driven Resonator
**Self Excited Loop

 
WE5RFP002 Design Status of Transfer Lines in TPS booster, linac, injection, storage-ring 2261
 
  • P.J. Chou, H.-P. Chang, C.-C. Kuo, W.T. Liu
    NSRRC, Hsinchu
 
 

The booster design of Taiwan Photon Source(TPS) has been significantly revised. Therefore, the transfer line from linac to booster(LTB) and the one from booster to storage ring(BTS) have been redesigned accordingly. The design of LTB transfer line has been simplified to reduce the number of magnets. The length of BTS transfer line has been greatly reduced. The design goal of transfer lines is to achieve high efficiency for beam injection. The status of current progress will be reported.

 
WE5RFP004 Study of Errors due to Utilization of the Transverse Deflectors in QBA Lattice of Taiwan Photon Source emittance, cavity, lattice, electron 2267
 
  • H. Ghasem, G.-H. Luo
    NSRRC, Hsinchu
 
 

Deflecting cavity generates a correlation between longitudinal position and vertical momentum of electrons in the synchrotron light sources for production short X-ray pulses. Use of such structures leads to growth in vertical amplitude and slope of stored electrons. Since errors are characteristic of real machine, any errors associated with the photon compression system must be considered and the tolerance of them must be evaluated. In this paper we present simulation of main errors due to deflecting structures, QBA lattice and injection system and find tolerances of them.

 
WE5RFP012 Analysis of the Orbit Response Matrix and Correction of Beta Function at the SAGA Light Source quadrupole, sextupole, power-supply, storage-ring 2291
 
  • Y. Iwasaki, T. Kaneyasu, S. Koda, Y. Takabayashi
    SAGA, Tosu
  • H. Ohgaki
    Kyoto IAE, Kyoto
 
 

The procedure of accelerator modeling using orbit response matrix fitting is well known and widely adopted at many light sources, we also examined the model fitting to diagnose optics and to restore the periodicity of the storage ring optics. In the modeling procedure we used the tracking code TRACY2, because it can calculate the orbit response matrix including energy offset caused by the dipole kick. The multi-parameter fitting was carried out by using SVD algorism implemented in the Labview mathematical package. In the fitting procedure, we fixed a steering magnet field to the value obtained from the orbit measurement using screen monitor to avoid explicit solution between the steering strengths and the BPM gains. By adopting the orbit response matrix fitting, it was found that the quadrupole strength is about 3-5% larger than the calculated value obtained from magnetic measurement data and output current of the power supply. In the conference, we will report on the result of the modeling procedure and its application to the optics correction.

 
WE5RFP028 Coherent Soft X-Ray Generation in the Water Window with the EEHG Scheme laser, FEL, radiation, bunching 2327
 
  • D. Xiang, G.V. Stupakov
    SLAC, Menlo Park, California
  • W.M. Fawley
    LBNL, Berkeley, California
 
 

Funding: This work was supported by U.S. DOE contracts DE-AC03-76SF00515 and under the auspices of the Office of Science, U.S. DOE under Contract No. DE-AC02-05CH11231.


Recently Stupakov* has suggested a scheme entitled echo-enabled harmonic generation (EEHG) for producing short wavelength FEL radiation that allows far higher harmonic numbers to be accessed as compared with the normal limit arising from incoherent energy spread. We have studied the feasibility of a single EEHG stage to generate coherent radiation in the "water window" (2- 4 nm wavelength) directly from a UV seed laser at ~200-nm wavelength. By adjusting the temporal overlap region of the two lasers producing energy modulation in the EEHG scheme, we find it may be possible to vary the duration of the output coherent soft x-ray pulse. We present time-dependent simulation results which explore these ideas and also examine the sensitivity of the scheme to various input electron beam parameters.


*G. Stupakov, Preprint SLAC-PUB-13445

 
WE5RFP029 Full Electromagnetic Simulation of Free-Electron Laser Amplifier Physics via the Lorentz-Boosted Frame Approach undulator, FEL, radiation, electron 2330
 
  • W.M. Fawley, J.-L. Vay
    LBNL, Berkeley, California
 
 

Funding: This work was supported under the auspices of the Office of Science, U.S. DOE under Contract No. DE-AC02-05CH11231.


Recently* it has been pointed out that numerical simulation of some systems containing charged particles with highly relativistic directed motion can by speeded up by orders of magnitude by choice of the proper Lorentz boosted frame. A particularly good example is that of short wavelength free-electron lasers (FELs) in which a high energy electron beam interacts with a static magnetic undulator. In the optimal boost frame with Lorentz factor gammaF, the red-shifted FEL radiation and blue shifted undulator have identical wavelengths and the number of required time-steps (presuming the Courant condition applies) decreases by a factor of gammaF-squared for fully electromagnetic simulation. We have adapted the WARP code** to apply this method to several FEL problems including coherent spontaneous emission (CSE) from pre-bunched e-beams, radiation in multi-wavelength undulators, and the effective lengths of undulators with entrance and exit matching ramps. We also discuss some preliminary results from applying the boosted-frame method to Coherent Synchrotron Radiation calculations.


*J.-L Vay Phys. Rev. Lett. 98, 130405 (2007)
**D.P. Grote, A. Friedman, J.-L. Vay, and I. Haber, AIP Conf. Proc., 749, 55 (2005).

 
WE5RFP037 A Simple, Low Cost Longitudinal Phase Space Diagnostic quadrupole, electron, diagnostics, emittance 2346
 
  • K.J. Bertsche, P. Emma
    SLAC, Menlo Park, California
  • O.A. Shevchenko
    BINP SB RAS, Novosibirsk
 
 

Funding: Work supported by the U.S. Department of Energy under contract number DE-AC02-76SF00515.


For proper operation of the LCLS x-ray free-electron laser, measurement and control of the electron bunch longitudinal phase space is critical. The LCLS accelerator includes two bunch compressor chicanes to magnify the peak current. These magnetic chicanes can generate significant coherent synchrotron radiation (CSR), which can distort the phase space distribution. We propose a diagnostic scheme by exciting a weak skew quadrupole at an energy-chirped, high dispersion point in the first bunch compressor (BC1) to reconstruct longitudinal phase space on an OTR screen after BC1, allowing a detailed characterization of the CSR effects.

 
WE5RFP040 Start-to-End Simulations of the LCLS Accelerator and FEL Performance at Very Low Charge FEL, emittance, linac, undulator 2355
 
  • Y.T. Ding, A. Brachmann, F.-J. Decker, D. Dowell, P. Emma, J.C. Frisch, A. Gilevich, G.R. Hays, P. Hering, Z. Huang, R.H. Iverson, H. Loos, A. Miahnahri, H.-D. Nuhn, D.F. Ratner, J.L. Turner, J.J. Welch, W.E. White, J. Wu
    SLAC, Menlo Park, California
  • C. Pellegrini
    UCLA, Los Angeles, California
 
 

The Linac Coherent Light Source (LCLS) is an x-ray Free-electron Laser (FEL) being commissioned at SLAC. Recent beam measurements have shown that, using the LCLS injector-linac-compressors, the beam emittance is very small at 20 pC*. A similar low charge operation mode was also suggested and studied**. In this paper we perform start-to-end simulations of the entire accelerator including the FEL undulator and study the FEL performance versus the bunch charge. At 20 pC charge, these calculations associated with the measured beam parameters suggest the possibility of generating a longitudinally coherent single x-ray spike with 2-femtosecond duration at a wavelength of 1.5 nm. At ~100 pC charge level, our simulations show an x-ray pulse with 20 femtosecond duration and up to 1012 photons at a wavelength of 1.5 Å. These results open exciting possibilities for ultrafast science and single shot molecular imaging.


*A. Brachmann et. al., to be published.
**J. Rosenzweig et al., Nuclear Instr. and Meth. A 593, 39-44 (2008); S. Reiche et al., Nucl. Instr. And Meth. A 593, 45-48 (2008).

 
WE5RFP057 Microbunching Gain of the Wisconsin FEL Beam Spreader impedance, FEL, linac, acceleration 2395
 
  • R.A. Bosch, K.J. Kleman
    UW-Madison/SRC, Madison, Wisconsin
  • J. Wu
    SLAC, Menlo Park, California
 
 

The microbunching gain of a free-electron laser (FEL) driver is affected by the beam spreader that distributes bunches to the FEL beam lines. For the Wisconsin FEL (WiFEL), analytic formulas and tracking simulations indicate that a beam spreader design with a low value of R56 has little effect upon the gain.

 
WE5RFP058 Single-Stage Bunch Compression for the Wisconsin FEL cavity, FEL, linac, electron 2398
 
  • R.A. Bosch, K.J. Kleman
    UW-Madison/SRC, Madison, Wisconsin
  • J. Wu
    SLAC, Menlo Park, California
 
 

The microbunching gain of the driver for the Wisconsin FEL (WiFEL) is reduced by more than an order of magnitude by using a single-stage bunch compressor rather than a two-stage design. This allows compression of a bunch with lower energy spread for improved FEL performance.

 
WE5RFP069 Electron Multipacting Can Explain the Pressure Rise in the ANKA Cold Bore Superconducting Undulator electron, vacuum, photon, undulator 2420
 
  • S. Casalbuoni, M. Hagelstein, D. Saez de Jauregui, S. Schleede
    FZK, Karlsruhe
 
 

Preliminary studies performed with the cold bore superconducting undulator installed in the ANKA storage ring suggest that the beam heat load is mainly due to the electron wall bombardment. Electron bombardment can both heat the cold vacuum chamber and induce an increase in the pressure because of gas desorption. In this contribution we compare the measurements of the pressure in a cold bore performed in the electron storage ring ANKA with the prediction obtained using the equations of gas dynamic balance in a cold vacuum chamber exposed to synchrotron radiation and electron bombardment. The balance results from two competitive effects: the photon and electron desorption of the gas contained in the oxide layer of the chamber wall and of the gas cryosorbed, and the cryopumping of the cold surface. We show that photodesorption alone cannot explain the pressure rise observed and that electron multipacting is needed.

 
WE5RFP076 Status of UCLA Helical Permanent-Magnet Undulator undulator, electron, laser, bunching 2441
 
  • A. Knyazik, J.B. Rosenzweig, R. Tikhoplav
    UCLA, Los Angeles
 
 

A helical undulator, utilizing permanent-magnet of cylindrically symmetric (Halbach) geometry has been developed at UCLA’s Neptune Facility. The initial prototype is a short 10 cm, 7 periods long helical undulator, designed to test the electron-photon coupling by observing the micro-bunching has been constructed and is currently being tested in the Neptune facility. An Open Iris-Loaded Waveguide Structure (OILS) scheme which conserves laser mode size and wave fronts throughout the undulator, is utilized to avoid Gouy phase shift caused by focusing of the drive laser. Coherent Transition Radiation and Coherent Cherenkov Radiation is used for micro-bunching diagnostic. Currently the undulator has been built, magnets were calibrated via pulsed wire method.

 
WE5RFP081 Development of an Electromagnetic/Permanent Magnet Helical Undulator for Fast Polarisation Switching permanent-magnet, undulator, power-supply, electron 2456
 
  • F. Marteau, P. Berteaud, F. Bouvet, L. Chapuis, M.-E. Couprie, J.P. Daguerre, J.-M. Filhol, A. Mary, K. Tavakoli
    SOLEIL, Gif-sur-Yvette
 
 

A new electromagnetic/permanent magnets helical undulator, with a 65 mm magnetic period is under development at SOLEIL for providing a rapid switching of the photon polarization required to perform dichroïsm experiments. The vertical field will be produced by coils fed by a fast switching power supply, with a maximum current of 350 A and a polarity switching time shorter than 100ms. The coils consist of copper sheets cut by water jet method. 26 layers of copper will be stacked together while 10 of them will be water cooled. The current-regulated power supply should be able to operate in the 4 quadrants with a 50 ppm current resolution over the full scale. The design of this home made power supply will be described. The horizontal field will be generated by NdFeB permanent magnets. The design vertical and horizontal peak field values in the helical configuration are 0.24 T at the minimum 15.5 mm gap. The magnetic design and the correction scheme will be described. A prototype was built to characterise and validate the technical choices, and the results will be discussed. The efficiency of the cooling system and the results of the magnetic measurements will be presented.

 
WE5RFP082 A Short Period Undulator Utilizing a Novel Material undulator, electron, laser, photon 2459
 
  • F.H. O'Shea, G. Marcus, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • J. Bahrdt, A. Gaupp
    BESSY GmbH, Berlin
  • F.J. Grüner, R. Weingartner
    LMU, München
 
 

The fundamentals of insertion device physics demand that to have access to ever higher photon energies either the beam energy must increase or the undulator period must decrease. Recent advances in accelerator technology have increased beam energies and at the same time insertion device technology has developed creative ways of producing light of the desired energy, characteristics and quality. This paper describes the simulation work for the design of a 9 mm period in-vacuum planar undulator using a new rare-earth magnetic material.

 
WE5RFP084 Spectral Characterisation of the ANKA-SCU Radiation undulator, radiation, electron, dipole 2465
 
  • A. Bernhard, T. Baumbach, F. Burkart, S. Ehlers, G. Fuchert, P. Peiffer, M. Wolf, D. Wollmann
    KIT, Karlsruhe
  • B. Kostka
    University of Erlangen-Nürnberg, Physikalisches Institut II, Erlangen
  • R. Rossmanith
    FZK, Karlsruhe
 
 

The ANKA superconductive undulator (SCU14) is continously operated since 2005. The main objetive of this operation was to investigate the interactions between the undulator and the stored electron beam and to characterise the undulator radiation. The characterisation of the undulator radiation was done with a short test beamline designed for spacially and spectrally resolved measurements of the undulator radiation intensity. This contribution summarises the results of these measurements. The spectra are cross-correlated with the magnetic field measurements carried out earlier.

 
WE5RFP085 Magnetic Field Transients in Superconductive Undulators undulator, coupling, electron, dipole 2468
 
  • S. Ehlers, T. Baumbach, G. Fuchert, P. Peiffer, D. Wollmann
    KIT, Karlsruhe
  • A. Bernhard, R. Rossmanith
    FZK, Karlsruhe
  • D. Schoerling
    IMFD, Freiberg
 
 

The next step towards introducing superconductive undulators as the new generation of insertion devices is to understand the impact of dynamic effects in the superconducting coils on the accelerator beam. These effects are seen as a temporal drift of the beam orbit, originating from transients of the magnetic field. The first systematic time resolved measurements of such drifts have been performed ANKA. Orbit displacement during several different ramping cycles, for different ramp rates and relaxation times, has been investigated. This contribution summarises the results of the measurements. The persistent current effects in the superconducting wires, as well as eddy currents in the yoke are discussed as possible sources for the transients.

 
WE6PFP004 Beam Dynamics and Expected RHIC Performance with 56 MHz RF Upgrade emittance, luminosity, cavity, ion 2483
 
  • A.V. Fedotov, I. Ben-Zvi
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


Recently, an upgrade of RHIC storage RF system with a superconducting 56 MHz cavity was proposed. This upgrade will provide significant increase in the acceptance of storage RF bucket. Presently, the short bunch length for collisions is obtained via RF gymnastics with bunch rotation (called “re-bucketing”), because the length of 197MHz bucket of 5 nsec is too short to accommodate long bunches otherwise. However, some increase in the longitudinal emittance occurs during re-bucketing. The 56MHz cavity will produce sufficiently short bunches which would allow one to operate without re-bucketing procedure. This paper summarizes simulation of beam evolution due to Intra-beam scattering (IBS) for beam parameters expected with the 56 MHz SRF cavity upgrade. Expected luminosity improvement is shown both for Au ions at 100 GeV/nucleon and for protons at 250 GeV.

 
WE6PFP005 IBS and Possible Luminosity Improvement for RHIC Operation below Transition Energy emittance, luminosity, injection, cavity 2486
 
  • A.V. Fedotov
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


There is a strong interest in low-energy RHIC collisions in the energy range below present RHIC transition energy. These collisions will help to answer one of the key questions in the field of QCD about the existence and location of a critical point on the QCD phase diagram. For low-energy RHIC operation, particle losses from the RF bucket are of particular concern since the longitudinal beam size is comparable to the existing RF bucket at low energies. However, operation below transition energy allows us to exploit an Intra-beam Scattering (IBS) feature that drives the transverse and longitudinal beam temperatures towards equilibrium by minimizing the longitudinal diffusion rate using a high RF voltage. Simulation studies were performed with the goal to understand whether one can use this feature of IBS to improve luminosity of RHIC collider at low-energies. This paper presents results of simulations which show that additional luminosity improvement for low-energy RHIC project may be possible with high RF voltage from a 56 MHz superconducting RF cavity that is presently under development for RHIC.

 
WE6PFP012 LHC Cleaning Efficiency with Imperfections collimation, alignment, beam-losses, closed-orbit 2504
 
  • C. Bracco, R.W. Assmann, S. Redaelli, Th. Weiler
    CERN, Geneva
 
 

The performance reach of the LHC depends on the magnitude of beam losses and the achievable cleaning efficiency of its collimation system. The ideal performance reach for the nominal Phase 1 collimation system is reviewed. However, unavoidable imperfections affect any accelerator and can further deteriorate the collimation performance. Multiple static machine and collimator imperfections were included in the LHC tracking simulations. Error models for collimator jaw flatness, collimator setup accuracy, the LHC orbit and the LHC aperture were set up, based to the maximum extent possible on measurements and results of experimental beam tests. It is shown that combined "realistic" imperfections can reduce the LHC cleaning efficiency by about a factor 11 on average.

 
WE6PFP018 Optimization of the LHC Separation Bumps Including Beam-Beam Effects emittance, beam-beam-effects, optics, luminosity 2522
 
  • S.M. White, H. Burkhardt, S.D. Fartoukh, T. Pieloni
    CERN, Geneva
 
 

The LHC beams will cross each other and experience perturbations as a result of the beam-beam effect at the interaction points, which can result in emittance growth and halo creation. The beam-beam force is approximately linear for small offsets and highly non-linear for larger offsets with peaks in growth close to 0.3 and 1.5 σ separation. We present a study of the process of going into collisions in the LHC and use simulations to investigate on possible emittance blow-up. We analyze how the crossing scheme can be optimized to minimize the collapsing time of the separation bumps for given hardware constraints.

 
WE6PFP021 First Beta-Beating Measurement in the LHC optics, coupling, quadrupole, injection 2531
 
  • R. Tomás, M. Aiba, S.D. Fartoukh, F. Franchi, M. Giovannozzi, V. Kain, M. Lamont, G. Vanbavinckhove, J. Wenninger, F. Zimmermann
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
  • A. Morita
    KEK, Ibaraki
 
 

In 2008 beam successfully circulated in the LHC. Thanks to an excellent functioning of the BPM system and the related software, injection oscillations were recorded for the first 90 turns at all BPMs. The analysis of these data gives the unique opportunity of evaluating the periodic optics and inferring possible error sources.

 
WE6PFP022 Beta-Beating Corrections in the SPS as a Testbed for the LHC optics, closed-orbit, betatron, sextupole 2534
 
  • R. Tomás, M. Aiba, G. Vanbavinckhove, J. Wenninger
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
  • A. Morita
    KEK, Ibaraki
 
 

For several years optics measurement and correction algorithms have been developed for the LHC. During 2008 these algorithms have been directly tested in the SPS and RHIC. The experimental results proving the readiness of the applications are presented.

 
WE6PFP024 ATF2 Ultra-Low IP Betas Proposal emittance, lattice, octupole, linear-collider 2540
 
  • R. Tomás, H.-H. Braun, J.-P. Delahaye, A. Marin, D. Schulte, F. Zimmermann
    CERN, Geneva
  • D. Angal-Kalinin, J.K. Jones
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • S. Bai, J. Gao, X.W. Zhu
    IHEP Beijing, Beijing
  • P. Bambade, M. Renier
    LAL, Orsay
  • Y. Honda, S. Kuroda, T. Okugi, T. Tauchi, N. Terunuma, J. Urakawa
    KEK, Ibaraki
  • A. Scarfe
    UMAN, Manchester
  • A. Seryi, G.R. White, M. Woodley
    SLAC, Menlo Park, California
 
 

The CLIC Final Focus System has considerably larger chromaticity than those of ILC and its scaled test machine ATF2. We propose to reduce the IP betas of ATF2 to reach a CLIC-like chromaticity. This would also allow to study the FFS tuning difficulty as function of the IP beam spot size. Both the ILC and CLIC projects will largely benefit from the ATF2 experience at these ultra-low IP betas.

 
WE6PFP025 Energy Deposition Patterns in the LHC Inner Triplet and Their Impact on the Phase II Luminosity Upgrade luminosity, quadrupole, shielding, focusing 2543
 
  • E.H.M. Wildner, F. Cerutti, A. Ferrari, A. Mereghetti, E. Todesco
    CERN, Geneva
  • F. Broggi
    INFN/LASA, Segrate (MI)
 
 

Recent studies show that the energy deposition for the LHC phase one luminosity upgrade, aiming at a peak luminosity 2.5 1034 cm-2s-1, can be handled by appropriate shielding. The phase II upgrade aims at a further increase of a factor 4, possibly using Nb3Sn quadrupoles. This paper describes how the main features of the triplet layout, such as quadrupole lengths, gaps between magnets, and aperture, affect the energy deposition in the insertion. We show the dependence of the triplet lay-out on the energy deposition patterns in the insertion magnets. An additional variable which is taken into account is the choice of conductor, i.e. solutions with Nb-Ti and Nb3Sn are compared. Nb3Sn technology gives possibilities for increasing the magnet apertures and space for new shielding solutions. Our studies give a first indication on the possibility of managing energy deposition for the phase II upgrade.

 
WE6PFP031 Simulations of Long-Range Beam-Beam Compensation in LHC dynamic-aperture, proton, beam-losses, betatron 2558
 
  • H.J. Kim, T. Sen
    Fermilab, Batavia
 
 

Abstract The compensation of long-range beam-beam interactions with current carrying wires in the Large Hadron Collider (LHC) is studied by multi-particle tracking. In the simulations, we include the effect of long-range collisions together with the nonlinearities of IR triplets, sextupoles, and head-on collisions. The model includes the wires placed at the locations reserved for them in the LHC rings. We estimate the optimal parameters of a wire for compensating the parasitic beam-beam force by long-term simulations of beam lifetime.

 
WE6PFP032 Beam-Beam Compensation Using Electron Lens in RHIC electron, proton, dynamic-aperture, betatron 2561
 
  • H.J. Kim, T. Sen
    Fermilab, Batavia
 
 

A beam-beam simulation code (BBSIMC) has been developed to study the interaction between counter moving beams in colliders and its compensation through a low energy electron beam. This electron beam is expected to improve intensity lifetime and luminosity of the colliding beams by reducing the betatron tune shift and spread from the head-on collisions. In this paper we discuss the results of beam simulations with the electron lens in the Relativistic Heavy Ion Collider (RHIC). We study the effects of the electron beam profile and strength on the betatron tunes, dynamic aperture, frequency diffusion and beam lifetime.

 
WE6PFP034 Electron Lens for Beam-Beam Compensation at LHC electron, beam-beam-effects, proton, emittance 2567
 
  • A. Valishev, V.D. Shiltsev
    Fermilab, Batavia
 
 

Funding: Work supported by the United States Department of Energy under Contract No. DE-AC02-07CH11359


Head-on beam-beam effect may become a major performance limitation for the LHC in one of the upgrade scenarios. Given the vast experience gained from the operation of Tevatron electron lenses, a similar device provides significant potential for mitigation of beam-beam effects at the LHC. In this report we present the results of simulation studies of beam-beam compensation and analyze potential application of electron lense at LHC and RHIC.

 
WE6PFP035 Suppression of Beam-Beam Tune Spread Using Hollow Electron Beam electron, proton, antiproton, gun 2570
 
  • A. Valishev, L.G. Vorobiev
    Fermilab, Batavia
 
 

Funding: Work supported by the United States Department of Energy under Contract No. DE-AC02-07CH11359


Significant difference in transverse size of the proton and antiproton bunches at collision points is known to cause deterioration of the larger (proton) beam life time at Tevatron. The reason is believed to be in the combination of large betatron tune spread induced by the high nonlinearity of the beam-beam force, and limited tune space. We consider the prospects for application of hollow electron beam for beam-beam tune spread suppression.

 
WE6PFP037 3D Strong-Strong Simulations of Wire Compensation of Long-Range Beam-Beam Effects at LHC emittance, beam-beam-effects, lattice, luminosity 2576
 
  • J. Qiang
    LBNL, Berkeley, California
 
 

Funding: Work supported by the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.


In this paper, we report on studying wire compensation of long-range beam-beam effects using a fully 3D strong-strong beam-beam model. The simulations include two head-on collisions with 0.3 mrad crossing angle and 64 long-range beam-beam collisions near IP 1 and IP5. We found that using conducting wires with appropriate current level will compensate the tail emittance growth due to long-range beam-beam effects. The random fluctuation of current level should be controlled below 0.1% level for a good compensation. Lowering the long-range beam-beam separations by 20% together with wire compensation will improve the luminosity by a few percentage. Further reducing the beam-beam separations causes significant beam blow-up and decrease of luminosity.

 
WE6PFP038 Strong-Strong Beam-Beam Simulation of Crab Cavity Compensation at LHC cavity, luminosity, emittance, collider 2579
 
  • J. Qiang
    LBNL, Berkeley, California
 
 

Funding: Work supported by the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.


Crab cavity is proposed to compensate the geometric luminosity loss of crossing angle collision at LHC upgrade. In this paper, we report on strong-strong beam-beam simulation of crab cavity compensation at LHC using the BeamBeam3D code. Simulation results showed that using a pair of local compensation for each beam could significantly improve the beam luminosity at collision. However, this improvement could be lost with random offset errors from the RF deflection cavities.

 
WE6PFP039 Emittance Growth due to Beam-Beam Effects with a Static Offset in Collision in the LHC emittance, proton, luminosity, beam-beam-effects 2582
 
  • T. Pieloni
    PSI, Villigen
  • W. Herr
    CERN, Geneva
  • J. Qiang
    LBNL, Berkeley, California
 
 

Under nominal operational conditions, the LHC bunches experience small unavoidable offset at the collision points caused by long range beam-beam interactions. Although the geometrical loss of luminosity is small, one may have to consider an increase of the beam transverse emittance, leading to a deterioration of the experimental conditions. In this work we evaluate and understand the dynamics of beam-beam interactions with static offsets at the collision point. A study of the emittance growth as a function of the offset amplitude in collisions is presented. Moreover, we address the effects coming from the beam parameters such as the initial transverse beam size, bunch intensity and tune.

 
WE6PFP043 Recent Progress of KEKB luminosity, coupling, cavity, sextupole 2588
 
  • Y. Funakoshi, T. Abe, K. Akai, Y. Cai, K. Ebihara, K. Egawa, A. Enomoto, J.W. Flanagan, H. Fukuma, K. Furukawa, T. Furuya, J. Haba, T. Ieiri, N. Iida, H. Ikeda, T. Kageyama, S. Kamada, T. Kamitani, S. Kato, M. Kikuchi, E. Kikutani, H. Koiso, M. Masuzawa, T. Mimashi, T. Miura, A. Morita, T.T. Nakamura, K. Nakanishi, M. Nishiwaki, Y. Ogawa, K. Ohmi, Y. Ohnishi, N. Ohuchi, K. Oide, M. Ono, Y. Seimiya, K. Shibata, M. Suetake, Y. Suetsugu, T. Sugimura, T. Suwada, M. Tawada, M. Tejima, M. Tobiyama, N. Tokuda, S. Uehara, S. Uno, Y. Yamamoto, Y. Yano, K. Yokoyama, M. Yoshida, S.I. Yoshimoto, D.M. Zhou
    KEK, Ibaraki
 
 

Crab cavities were installed at KEKB at the beginning of 2007. The beam operation with the crab cavities is in progress. In this paper, machine performance with crab crossing is described focusing on a specific luminosity and a beam lifetime issue related to the dynamic beam-beam effects.

 
WE6PFP045 Beam Dynamics for Very High Beam-Beam Parameter in an e+e- Collider collider, cavity, luminosity, betatron 2592
 
  • K. Ohmi, K. Oide
    KEK, Ibaraki
 
 

Beam-beam tune shift parameter characterizes the strength of the nonlinear interaction due to the beam-beam collision. The tune shift has been measured in many e+e- colliders and has been an indicator for the collider performance. The record for the tune shift is known as 0.07-0.1 depending on the parameter of the collider, especially the radiation damping rate. We discuss the fundamental limit of the tune shift can be very high (>0.2) depending on the choice of collider parameter, which concerns operating point near the half integer tune, head-on collision and travel focus.

 
WE6PFP049 Crab Waist Collision Scheme: Numerical Simulations versus Experimental Results luminosity, lattice, sextupole, collider 2604
 
  • P.A. Piminov, E.B. Levichev, D.N. Shatilov
    BINP SB RAS, Novosibirsk
  • C. Milardi, M. Zobov
    INFN/LNF, Frascati (Roma)
  • K. Ohmi
    KEK, Ibaraki
 
 

A novel scheme of crab waist collisions has been successfully tested at the electron-positron collider DAΦNE, Italian Phi-factory. In this paper we compare numerical simulations of the crab waist beam-beam interaction with obtained experimental results. For this purpose we perform weak-strong and quasi strong-strong beam-beam simulations using a realistic DAΦNE lattice model that has proven to reproduce reliably both linear and nonlinear collider optics.

 
WE6PFP055 Observation and Simulation of Beam-Beam Induced Emittance Growth in RHIC emittance, luminosity, proton, collider 2622
 
  • J. Beebe-Wang, S.Y. Zhang
    BNL, Upton, Long Island, New York
 
 

Funding: Work performed under the auspices of the US DOE.


In the recent years the peak luminosity of the RHIC polarized proton run has been improved. However, as a consequence, the luminosity lifetime is reduced. The beam emittance growth during the beam storage is a main contributor to the luminosity lifetime reduction, and it seems to be caused mainly by the beam-beam effect during collision. It is, therefore, important to better understand the beam-beam collision effects in RHIC with the aid of particle tracking codes. A simulation study of the emittance growth is performed with RHIC machine parameters using the LIFETRAC code*. The initial results of this study were reported in an earlier paper**. In order to achieve a better understanding and to provide guidance for future RHIC operations, we present an in depth investigation of the emittance growth for a range of RHIC operation tunes, bunch lengths and initial emittance. The simulation results are also compared to the available data from experimental measurements.


*D.Shatilov, et al.,"Lifetrac Code for the Weak-Strong Simulation of the Beam-Beam Effects in Tevatron",PAC05 proc.
**J.Beebe-Wang,“Emittance Growth due to Beam-Beam Effect in RHIC”,PAC07 Proc.

 
WE6PFP065 Recent Progress on Design Studies of High-Luminosity Ring-Ring Electron-Ion Collider at CEBAF electron, ion, luminosity, polarization 2652
 
  • Y. Zhang, S.A. Bogacz, A. Bruell, P. Chevtsov, Y.S. Derbenev, R. Ent, G.A. Krafft, R. Li, L. Merminga, B.C. Yunn
    JLAB, Newport News, Virginia
 
 

Funding: Authored by Jefferson Science Associates, LLC under U.S. DOE Contract No. DE-AC05-06OR23177.


The conceptual design of a ring-ring electron-ion collider based on CEBAF has been continuously optimized to cover a wide center-of-mass energy region and to achieve high luminosity and polarization to support next generation nuclear science programs. Here, we summarize the recent design improvements and R&D progress on interaction region optics with chromatic aberration compensation, matching and tracking of electron polarization in the Figure-8 ring, beam-beam simulations and ion beam cooling studies.

 
WE6PFP067 Simulation Studies of Beam-Beam Effects of a Ring-Ring Electron-Ion Collider Based on CEBAF electron, luminosity, proton, collider 2653
 
  • Y. Zhang
    JLAB, Newport News, Virginia
  • J. Qiang
    LBNL, Berkeley, California
 
 

Funding: (1) Authored by Jefferson Science Associates, LLC under U.S. DOE Contract No. DE-AC05-06OR23177 (2) Supported by the U. S. Department of Energy under Contract no. DE-AC02-05CH11231.


The collective beam-beam effect can potentially cause a rapid growth of beam sizes and reduce the luminosity of a collider to an unacceptably low level. The ELIC, a proposed ultra high luminosity electron-ion collider based on CEBAF, employs high repetition rate crab crossing colliding beams with very small bunch transverse sizes and very short bunch lengths, and collides them at up to 4 interaction points with strong final focusing. All of these features can make the beam-beam effect challenging. In this paper, we present simulation studies of the beam-beam effect in ELIC using a self-consistent strong-strong beam-beam simulation code developed at Lawrence Berkeley National Laboratory. This simulation study is used for validating the ELIC design and for searching for an optimal parameter set.

 
WE6PFP068 Emittance Evolution of the Drive Electron Beam in a Helical Undulator for ILC Positron Source undulator, emittance, electron, damping 2656
 
  • W. Gai, M. Borland, K.-J. Kim, W. Liu, A. Xiao
    ANL, Argonne
  • J. Sheppard
    SLAC, Menlo Park, California
 
 

Funding: This work was supported by the US Department of Energy Office of Science under Contract No. DE-AC02-06CH11357.


The effect of ILC positron source’s helical undulator to the drive electron beam is of great interest. People have been looking into the effect of wakefield, quad misalignment and also the effect of radiation. In this paper we’ll report an emittance damping effect of the ILC positron source undulator to the drive electron beam and our QUAD-BPM error simulation results. For 100m RDR undulator, the emittance of drive electron beam will be damped down by about 1% instead of growing as the damping is stronger than quantum excitation for this RDR undulator with the RDR drive electron beam. Quad-BPM misalignment simulations show that a 20um rms misalignment error in a 250m long undulator beamline can cause about 5% emittance growth in drive electron beam. Taking into consider the damping effect of undulator, the net emittance growth will be smaller.

 
WE6PFP071 ATF2 Spot Size Tuning Using the Rotation Matrix Method sextupole, quadrupole, extraction, coupling 2662
 
  • A. Scarfe, R. Appleby
    UMAN, Manchester
  • D. Angal-Kalinin, J.K. Jones
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

The Accelerator Test Facility (ATF2) at KEK aims to experimentally verify the local chromaticity correction scheme to achieve a vertical beam size of 37nm. The facility is a scaled down version of the final focus design proposed for the future linear colliders. In order to achieve this goal, high precision tuning methods are being developed. One of the methods proposed for ATF2 is a novel method known as the ‘rotation matrix’ method. Details of the development and testing of this method, including orthogonality optimisation and simulation methods, are presented.

 
WE6PFP074 Failures in the Main Linac of the International Linear Collider and their Effect on the Beam Delivery System quadrupole, beam-losses, linac, klystron 2667
 
  • I. Melzer-Pellmann, D. Kruecker, F. Poirier, N.J. Walker
    DESY, Hamburg
 
 

Funding: This work is supported by the Commission of the European Communities under the 6th Framework Programme "Structuring the European Research Area", contract number RIDS-011899.


The International Linear Collider (ILC) relies on very high beam powers and very small beam emittance to achieve the ambitious luminosity of 2·10+34 cm-2s-1. The potential for damage to the accelerator hardware in the event of some machine failure will require a sophisticated machine protection system. The small apertures in the Beam Delivery System (BDS) - specifically the collimators (by definition the smallest apertures in the machine) are particularly critical. Possible failures in the Main Linac of the ILC and their impact on the BDS are studied using the MERLIN C++ library*. We show that the machine is safe for at least one bunch in case of one of the described failures; a fast abort system is designed to safely extact the remainder of the bunches in the pulse to a dump. Investigated are phase and voltage shifts of the klystrons, quadrupole and corrector coil failures.


*Merlin - A C++ Class Library for Accelerator Simulations; http://www.desy.de/~merlin.

 
WE6PFP075 Effect of the Non-Linear Magnetic Fields on the Emittance Growth in the ATF Extraction Line emittance, extraction, quadrupole, multipole 2670
 
  • M. Alabau, P. Bambade, G. Le Meur, F. Touze
    LAL, Orsay
  • A. Faus-Golfe
    IFIC, Valencia
  • S. Kuroda
    KEK, Ibaraki
  • M. Woodley
    SLAC, Menlo Park, California
 
 

Since several years, the vertical beam emittance measured in the Extraction Line (EXT) of the Accelerator Test Facility (ATF) at KEK, has been significantly larger than that measured in the damping ring (DR) itself. The EXT line that transports the beam to the ATF2 Final Focus beam line has been rebuilt, but the extraction itself remains in most part unchanged, with the extracted beam transported off-axis horizontally in two of the quadrupoles, beyond the linear region for one of them. A few other nearby magnets have also modelled or measured non-linearity. In case of a residual vertical beam displacement, this can result in increased vertical emittance through coupling between the two transverse planes. Tracking studies as well as measurements have been carried out to study this effect and the induced sensitivity of beam optical parameters to the trajectory at injection, in view of deriving tolerances for reproducible and stable operation.

 
WE6PFP085 Halo and Tail Simulations with Application to the CLIC Drive Beam scattering, electron, radiation, ion 2700
 
  • M. Fitterer, A.-S. Müller
    KIT, Karlsruhe
  • E. Adli, H. Burkhardt, B. Dalena, G. Rumolo, D. Schulte
    CERN, Geneva
  • I. Ahmed
    NCP, Islamabad
  • A. Latina
    Fermilab, Batavia
 
 

We report about generic halo and tail simulations and estimates. Previous studies were mainly focused on very high energies as relevant for the beam delivery systems of linear colliders. We have now studied, applied and extended these simulations to lower energies as relevant for the CLIC drive beam.

 
WE6PFP087 Muon Ionisation Cooling in Reduced RF cavity, factory, solenoid, scattering 2706
 
  • C.T. Rogers
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • G. Prior
    CERN, Geneva
 
 

In Muon Ionisation Cooling, closely packed high-field RF cavities are interspersed with energy-absorbing material in order to reduce particle beam emittance. Transverse focussing of the muon beams is achieved by superconducting magnets. This results in the RF cavities sitting in intense magnetic fields. Recent studies have shown that this may limit the peak gradient that can be achieved in the RF cavities. In this paper, we study the effect that a reduced RF gradient may have on the cooling performance of the Neutrino Factory lattice and examine methods to mitigate the effect.

 
WE6PFP089 Muon Capture, Phase Rotation, and Precooling in Pressurized RF Cavities cavity, factory, solenoid, emittance 2712
 
  • D.V. Neuffer
    Fermilab, Batavia
  • C.M. Ankenbrandt, R.P. Johnson, C. Y. Yoshikawa
    Muons, Inc, Batavia
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-05ER86252 and FRA DOE contract number DE-AC02-07CH11359


Gas-filled RF cavities can provide high-gradient accelerating fields for muons, and can be used for simultaneous acceleration and cooling of muons. In this paper we explore using these cavities in the front-end of the capture and cooling systems for neutrino factories and muon colliders. We consider using gas-filled RF cavities for the initial front end cooling systems. We also consider using them for simultaneous phase-energy rotation and cooling in a front-end system. We also consider using lower-density RF cavities, where the gas density is primarily for RF breakdown suppression, with less cooling effect. Pressurized RF cavities enable higher gradient rf within magnetic fields than is possible with evacuated cavities, enabling more options in the front-end. The status of designs of the capture, phase rotation, and precooling systems of muon beams in pressurized cavities is described.

 
WE6PFP093 Reverse Emittance Exchange for Muon Colliders emittance, resonance, collider, betatron 2721
 
  • V. Ivanov, A. Afanasev, C.M. Ankenbrandt, R.P. Johnson, G.M. Wang
    Muons, Inc, Batavia
  • S.A. Bogacz, Y.S. Derbenev
    JLAB, Newport News, Virginia
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-05ER86253


Muon collider luminosity depends on the number of muons in the storage ring and on the transverse size of the beams in collision. Six-dimensional cooling schemes now being developed will reduce the longitudinal emittance of a muon beam so that smaller high frequency RF cavities can be used for later stages of cooling and for acceleration. However, the bunch length at collision energy is then shorter than needed to match the interaction region beta function. New ideas to shrink transverse beam dimensions by lengthening each bunch (reverse emittance exchange and bunch coalescing) will help achieve high luminosity in muon colliders with fewer muons. Analytic expressions for the reverse emittance exchange mechanism are derived, including a new resonant method of beam focusing. Correction schemes for the aberrations were explored, and a lattice to implement them was proposed. To mitigate space charge detuning and wake field effects, a scheme was invented to coalesce smaller intensity bunches after they are cooled and accelerated to high energy into intense bunches suitable for a muon collider.

 
WE6PFP095 Integrating the MANX 6-D Muon Cooling Experiment with the MICE Spectrometers solenoid, emittance, cavity, dipole 2727
 
  • S.A. Kahn, R.J. Abrams, C.M. Ankenbrandt, M.A.C. Cummings, R.P. Johnson, T.J. Roberts
    Muons, Inc, Batavia
  • K. Yonehara
    Fermilab, Batavia
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-06ER86282


The MANX experiment is to demonstrate the reduction of 6D muon phase space emittance using a continuous liquid absorber to provide ionization cooling in a helical solenoid magnetic channel. The experiment involves the construction of a short two-period long helical cooling channel (HCC) to reduce the muon invariant emittance by a factor of two. The HCC would replace the current cooling section of the MICE experiment now being setup at the Rutherford Appleton Laboratory. The MANX experiment would use the existing MICE spectrometers and muon beam line. This paper shall consider the various approaches to integrate MANX into the RAL hall using the MICE spectrometers. This study shall discuss the matching schemes used to minimize losses and prevent emittance growth between the MICE spectrometers and the MANX HCC. Also the placement of additional detection planes in the matching region and the HCC to improve the resolution will be examined.

 
WE6PFP096 Particle Refrigerator ion, electron, emittance, solenoid 2730
 
  • T.J. Roberts
    Muons, Inc, Batavia
  • D.M. Kaplan
    Illinois Institute of Technology, Chicago, Illinois
 
 

Funding: Work supported in part by USDOE STTR Grant DE FG02 08ER86281.


We describe an approach that can extend the utility of frictional cooling, originally developed for muon beams, to other particles and ions, producing beams of exceptionally low normalized emittance. Moreover, via this approach the small momentum acceptance typical of frictional cooling channels can be increased by two to three orders of magnitude, making it possible to handle much larger intensities with much higher transmission, while preserving the exceptionally low normalized emittance of the output. Simulation studies have been used to optimize the design and performance for a variety of ions and particles, and an inexpensive experiment has been designed to test and verify the concept and simulations, using alpha particles from a radioactive source.

 
WE6PFP101 The Study of a Li Lens System as a Final Cooler for a Muon Collider collider, solenoid, emittance, focusing 2745
 
  • D.B. Cline, X.P. Ding, A.A. Garren, K.K. Lee
    UCLA, Los Angeles, California
 
 

We describe the Li Lens concept for a cooler for the transverse emittance for a μ+μ- collider. Different configurations are discussed such as Linear Cooler, Ring Coolers all with Li Lens inserts. We then describe a program to study the construction of Liquid Li Lens and a possible experiment at FNAL.

 
WE6PFP108 Beam Based Calibration of Slow Orbit Bump at NSLS Booster extraction, booster, dipole, septum 2763
 
  • X. Yang, J. Rose, T.V. Shaftan
    BNL, Upton, Long Island, New York
 
 

The orbit bumps in NSLS booster are used to move the beam orbit within 2mm to the extraction septum aperture in a time scale of millisecond at extraction in order to reduce the required strength of the fast extraction kicker. Since before extraction, the beam stays on the distorted orbit for thousands of revolutions, there is a concern that this may cause charge losses. In order to find the optimal orbit bump setpoint which brings the maximum distortion at the extraction position and minimum distortions at other places, we developed the extraction model and performed an experiment to validate it. Afterwards, the model was applied to optimize the extraction process.

 
WE6RFP008 Design of a 1.3 GHZ Single 9 Cell SC Cavity Test Cryomodule for ILC Collaboration at IHEP cryomodule, cavity, cryogenics, radiation 2796
 
  • T.X. Zhao, W.H. Lu, L.-Y. Xiong, L. Zhang, Z.G. Zong
    TIPC, BeiJing
  • J. Gao, Y. Sun, J.Y. Zhai
    IHEP Beijing, Beijing
  • Z.L. Hou, C.H. Li
    IHEP Beiing, Beijing
  • L.Q. Liu
    Technical Institute of Physics and Chemistry, Beijing
  • T.X. Zhao
    Graduate School of the Chinese Academy of Sciences, Beijing
 
 

Funding: Work supported by NSFC 10525525


In order to obtain the design, manufacture and operational experiences on the SRF cryomodule toward ILC, a test cryomodule for 1.3GHz single 9-cell SC cavity was designed by IHEP (Institute of High Energy Physics) and TIPC (Technical Institute of Physics and Chemistry) jointly. This cryomodule will be used as a 1.3GHz 9 cell SC cavity horizontal test facility. The cryogenic system for the cryomodule is designed and will be operated at 2.0K, with the saturated superfluid helium. The major requirements, design, simulation results of the cryomodule are reported in the paper. This key component of a superconducting accelerator test unit will be built in the near future at IHEP.

 
WE6RFP012 Simulation of the LHC Collimation System Using MERLIN collimation, scattering, wakefield, storage-ring 2805
 
  • H.L. Owen, S. Alshammari, R. Appleby, R.J. Barlow, A.M. Toader
    UMAN, Manchester
 
 

The LHC Collimators are designed to remove halo particles such that they do not impinge onto either detectors or other vulnerable regions of the storage ring. However, the very high 7 TeV energy means that their design is critical, as is the modelling of the absorption, scattering and wakefield effects upon the passing bunches. Existing simulations are being performed using Sixtrack and K2. We compare these simulations with results obtained using the MERLIN code, which includes a fuller description of the scattering and wakefield processes.

 
WE6RFP019 Simulation Results for Crystal Collimation Experiment in SPS UA9 proton, scattering, lattice, octupole 2823
 
  • E. Laface, W. Scandale
    CERN, Geneva
  • G. Cavoto
    INFN-Roma, Roma
  • S. Peggs
    BNL, Upton, Long Island, New York
 
 

The UA9 experiment will take place in 2009 at the CERN-SPS and will evaluate the feasibility of silicon crystals as primary collimators for a storage ring. A crystal placed at 6 σ from the beam core will deviate protons towards two roman pots and a tungsten absorber (TAL). In this paper the authors show simulations of the expected beam dynamics and of the capture efficiency into the secondary collimator. The result of these simulations will guide us in interpreting the experimental data expected in UA9.

 
WE6RFP021 Beam Loss Predictions for the UA9 Crystal Collimation Experiment beam-losses, collimation, quadrupole, optics 2829
 
  • V.P. Previtali, R.W. Assmann, S. Redaelli
    CERN, Geneva
  • V.P. Previtali
    EPFL, Lausanne
  • I.A. Yazynin
    IHEP Protvino, Protvino, Moscow Region
 
 

The UA9 experiment at the SPS aims at testing bent crystals for usage as collimators with high energy stored proton and heavy ion beams. The experiments will try to establish crystal-based cleaning efficiency with slowly diffusing beam halo. One method for evaluating efficiency relies on Roman Pots and is described elsewhere. An alternative method relies on observing the beam loss signals around the ring. Comparisons of losses escaping from standard collimators and bent crystals will allow determination of cleaning efficiency, equivalent to the definition used for the LHC collimation design. This alternative method is described and simulations with LHC collimation tracking tools for UA9 are discussed. The predicted beam losses along the SPS ring are presented for different orientations and amorphous layer thicknesses of the crystal. The effect of different diffusion speeds for the beam are discussed.

 
WE6RFP022 Simulations of Crystal Collimation for the LHC collimation, insertion, alignment, betatron 2832
 
  • V.P. Previtali, R.W. Assmann, S. Redaelli
    CERN, Geneva
  • V.P. Previtali
    EPFL, Lausanne
  • I.A. Yazynin
    IHEP Protvino, Protvino, Moscow Region
 
 

Bent crystals are promised to provide a path towards significant improvement of cleaning efficiency for high power collimation systems. In this paper a possible implementation of a crystal-enhanced collimation system is evaluated for the LHC. Simulation studies were performed with the same state-of the art tracking codes as used for the design of the conventional LHC collimation system. The numerical models are described and predictions for the local and global cleaning efficiency with a crystal-based LHC collimation system are presented. Open issues and further work towards a crystal collimation design for the LHC are discussed.

 
WE6RFP028 ISOL Target-Vapor Transport System Simulations target, ISOL, ion, vacuum 2850
 
  • Y. Zhang, Z. Liu, R. Remec
    ORNL, Oak Ridge, Tennessee
 
 

Funding: *SNS is managed by UT-Battelle, LLC, under contract DE-AC05-00OR22725 for the U.S. Department of Energy


The combined time required for diffusion release from target materials and effusive-flow of short-lived ion species must be minimized at ISOL based radioactive ion beam (RIB) facilities. Computational simulation studies with state-of-the-art codes offer cost effective means for designing targets with optimized diffusion release properties and vapor transport systems with short path lengths, as required for such applications. To demonstrate the power of the technique for designing optimum thickness targets, analytic solutions to the diffusion equation are compared with those obtained from a finite-difference code for radioactive particle release from simple geometries. The viability of the Monte Carlo technique as a practical means for optimally designing vapor transport systems is demonstrated by simulating the effusive-flow of neutral particles through several complex vapor transport systems. Important issues which affect the yield rates of short-lived species generated in high power ISOL targets are also discussed.

 
WE6RFP031 Prospects for Integrating a Hollow Electron Lens into the LHC Collimation System electron, collimation, proton, resonance 2856
 
  • J.C. Smith
    SLAC, Menlo Park, California
  • R.W. Assmann, V.P. Previtali
    CERN, Geneva
  • V.D. Shiltsev, A. Valishev
    Fermilab, Batavia
 
 

Funding: Work supported in part by the U.S. Department of Energy contract DE-AC02-76SF00515


It has been proposed to use a hollow electron lens with the LHC beam collimation system*. The hollow electron beam would be used as a beam scraper and positioned at a closer σ than the primary collimators to increase the halo particle diffusion rate striking the primaries. In this paper we use multi-turn beam tracking simulations to analyze the effectiveness of such a lens when integrated into the LHC collimation system.


*Shiltsez, V. et al. "LHC Particle Collimation by Hallow Electron Beams," Proceedings EPAC08, MOPC098 (2008)

 
WE6RFP033 Design and Development of the T2K Pion Production Target target, proton, radiation, factory 2860
 
  • C.J. Densham, M. Baldwin, M.D. Fitton, V.B. Francis, M.T. Rooney, M.L. Woodward
    STFC/RAL, Chilton, Didcot, Oxon
  • A. Ichikawa
    Kyoto University, Kyoto
  • T. Nakadaira, T. Sekiguchi
    KEK, Ibaraki
 
 

Funding: Science and Technology Facilities Council


The T2K experiment will utilise the highest pulsed power proton beam ever built to generate an intense beam of neutrinos. This uses the conventional technique of colliding the 0.75 MW 30 GeV proton beam with a graphite target and using a magnetic horn system to collect pions of one charge and focus them into a decay volume where the neutrino beam is produced. The target is a two interaction length (900 mm long) graphite target supported directly within the bore of the first magnetic horn which generates the required field with a pulsed current of 300 kA. This paper describes the design and development of the target system required to meet the demanding requirements of the T2K facility. Challenges include radiation damage, shock waves resulting from a 100 K temperature rise in the graphite material during each beam spill, design and optimisation of the helium coolant flow, and integration with the pulsed magnetic horn. Conceptual and detailed engineering studies were required to develop a target system that could satisfy these requirements and could also be replaced remotely in the event of a target failure.

 
WE6RFP034 Beam Impact Studies for ILC Collimators electron, vacuum, laser, target 2863
 
  • G. Ellwood
    STFC/RAL, Chilton, Didcot, Oxon
  • J.-L. Fernandez-Hernando
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • M. Slater, N.K. Watson
    Birmingham University, Birmingham
 
 

Spoilers in the ILC Beam Delivery System are required to survive without failure a minimum of 1-2 direct impacts of 250 GeV-500 GeV bunch of electrons or positrons, in addition to maintaining low geometric and resistive wall wake fields. The likelihood of spoiler survival was determined using finite element models of thermal and mechanical properties of the spoilers, with realistic patterns of energy deposition as input. The second phase of an experiment to calibrate the finite element models using electron beam data will be performed in the ATF2 extraction line, by subjecting a small sample of Ti-6Al-4V to bunches of electrons. The displacement of the surface will be measured with a Velocity Interferometer System of Any Reflector (VISAR). This paper shows the project plan as well as results of the simulations and expected readout from the VISAR.

 
WE6RFP036 Activation and Residual Equivalent Dose Rate Studies for an ILC Betatron Spoiler Prototype shielding, photon, wakefield, electron 2869
 
  • J.-L. Fernandez-Hernando
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

Funding: This work is supported by the Commission of the European Communities under the 6th Framework Programme “Structuring the European Research Area”, contract number RIDS-011899


After different wakefield test beams and radiation damage studies a prototype design for the International Linear Collider (ILC) spoilers of the betatron collimation system in the Beam Delivery System (BDS) is under development. Studies of activation and residual equivalent dose rate are needed in order to achieve an optimum design as well as to assess the radiation shielding requirements.

 
WE6RFP038 A FEA Study of the Stress Waves Generated in the T2K Beam Window from the Interaction with a High Power Pulsed Proton Beam proton, target, vacuum, resonance 2875
 
  • M.T. Rooney, C.J. Densham
    STFC/RAL, Chilton, Didcot, Oxon
  • Y. Yamada
    KEK, Ibaraki
 
 

The target station of the T2K neutrino facility requires a beam window to separate the target chamber, containing helium at atmospheric pressure, from the secondary beam line, which is maintained at ultra high vacuum. In addition to withstanding this differential pressure, the window must survive induced stresses due to intense heating resulting from interaction with a 0.75 MW pulsed proton beam. The design consists of a hemispherical double window with forced convection helium cooling in the volume enclosed, manufactured from titanium alloy. Preliminary analysis suggested that 'shock' waves induced by the pulsed nature of the beam will form the dominant mode of stress. The finite element software ANSYS Mechanical (V10) has been used to simulate the effect of beam impingement on a variety of window thicknesses in an attempt to find the optimum geometry. Results have shown that through thickness stress waves can be amplified if successive bunches arrive in phase with the waves generated by previous bunches. Therefore, thickness has been shown to be a critical variable in determining the window’s resistance to induced thermal shock.

 
WE6RFP042 The FERMI@elettra Beam Dump electron, emittance, FEL, linac 2887
 
  • S. Ferry, E. Karantzoulis
    ELETTRA, Basovizza
 
 

Funding: The work was supported in part by the Italian Ministry of University and Research under grant FIRB-RBAP045JF2.


The FERMI@elettra electron beam dump is designed for a 1nC, 1.8 GeV, 50Hz repetition rate beam. Using GEANT simulations, materials are chosen to absorb 99% of the beam energy and to limit the radio-isotope production. In addition, from the energy deposition distribution inside the dump, the thermal load is estimated. The necessary requirements, the design and the expected performance are presented and discussed.

 
WE6RFP043 FERMI@elettra Collimators electron, wakefield, undulator, collimation 2890
 
  • S. Ferry, C. Bontoiu, P. Craievich, S. Di Mitri, E. Karantzoulis
    ELETTRA, Basovizza
 
 

Funding: The work was supported in part by the Italian Ministry of University and Research under grant FIRB-RBAP045JF2.


To avoid damages on permanent magnets by the electrons, collimators will be installed in FERMI@elettra. Their dimensions and shape are defined through the beam optics and the induced wake fields while GEANT simulations are performed to determine their absorption efficiency and thermal load for both normal operating conditions and in case of miss-steering. The design, the simulations and the expected performance of the collimators are presented and discussed.

 
WE6RFP049 Optimisation of the Powering Tests of the LHC Superconducting Circuits extraction, quadrupole, cryogenics, dipole 2908
 
  • B. Bellesia, M.P. Casas Lino, R. Denz, C. Fernandez-Robles, M. Pojer, R.I. Saban, R. Schmidt, M. Solfaroli Camillocci, H. Thiesen, A. Vergara-Fernández
    CERN, Geneva
 
 

The Large Hadron Collider has 1572 superconducting circuits which are distributed along the eight 3.5 km LHC sectors. Time and resources during the commissioning of the LHC technical systems were mostly consumed by tests of each circuit of the collider: the powering tests. The tests consisted in carrying out several powering cycles at different current levels for each superconducting circuit. The Hardware Commissioning Coordination was in charge of planning, following up and piloting the execution of the test program. The first powering test campaign was carried out in summer 2007 for sector 7-8 with an expected duration of 12 weeks. The experience gained during these tests was used by the commissioning team for minimising the duration of the following powering campaigns to comply with the stringent LHC Project deadlines. Improvements concerned several areas: strategy, procedures, control tools, automatisation, resource allocation led to an average daily test rate increase from 25 to 200 tests per day. This paper describes these improvements and details their impact on the operation during the last months of LHC Hardware Commissioning.

 
WE6RFP050 The Conceptual Design of TPS Grounding System site, storage-ring, electron, controls 2911
 
  • T.-S. Ueng, J.-C. Chang, Y.-C. Lin, H.S. Wang
    NSRRC, Hsinchu
 
 

The TPS (Taiwan Photon Source) of NSRRC is in the design stage now. The grounding system is crucial to the safety issue, the electrical reference level, the electrical noise and the EMI problems. In order to provide a high quality electrical environment, the grounding system should be designed carefully. The soil resistivity of the construction site was investigated first. Many different configurations of the ground grid layouts were simulated and compared. Beside the horizontal ground-conductors, the vertical ground-electrodes of 30 m are considered to be installed below the ground surface and they will reach the ground water level in hopes of minimizing the resistance of ground grid. The main goal is to obtain a ground grid with resistance lower than 0.2 ohm. A rectangular ground grid will also be installed under the new utility building. It will be connected to the ground grid of TPS to further reduce the resistance of whole grounding system, and also to eliminate the potential difference between them.

 
WE6RFP051 Numerical Simulation of the Air Conditioning System Design for the 3 GeV TPS Storage Ring storage-ring, booster, controls, radiation 2914
 
  • J.-C. Chang, Y.-C. Chung, C.Y. Liu, A. Sheng, Z.-D. Tsai, T.-S. Ueng
    NSRRC, Hsinchu
 
 

The air conditioning system for the 3.0 GeV Taiwan Photon Source (TPS) is currently under the design phase. This paper presents the latest design of the air conditioning system for the TPS. The capacity of the air handling unit (AHU), the dimension and layout of the wind duct were specified. Numerical analysis was applied to simulate the air flow and temperature distribution in one of 24 sections storage ring. A 1/12 experimental hall was also modelled. The air flow of this area was simulated.

 
WE6RFP056 Development of a Non-Axisymmetric Permanent Magnet Focusing System for Elliptic Charged-Particle Beams cathode, electron, gun, focusing 2926
 
  • T.M. Bemis, M.H. Lawrence, J.Z. Zhou
    Beam Power Technology, Inc., Chelmsford, MA
  • C. Chen
    MIT/PSFC, Cambridge, Massachusetts
 
 

Funding: This work was funded in part by the Department of Energy, Grant No. DE-FG02-07ER84910 and Grant No. DE-FG02-95ER40919, and the MIT Deshpande Center for Technological Innovation.


High-brightness space-charge-dominated elliptic electron or ion beams have wide applications in high-power rf sources, particle accelerators, and/or ion implantation. Building upon recent inventions and theoretical studies on the generation and transport of elliptic charged-particle beams, a basic research and development program is being carried out to experimentally demonstrate a high-brightness, space-charge-dominated elliptic electron beam using a non-axisymmetric permanent magnet focusing system and an elliptic electron gun. Results of the design of such an elliptic electron beam system are presented.

 
WE6RFP060 A 26 GHz Dielectric Based Wakefield Power Extractor wakefield, vacuum, coupling, electron 2930
 
  • C.-J. Jing, F. Gao, A. Kanareykin, A.L. Kustov, P. Schoessow
    Euclid TechLabs, LLC, Solon, Ohio
  • M.E. Conde, W. Gai, R. Konecny, J.G. Power
    ANL, Argonne
  • S. Kazakov
    KEK, Ibaraki
 
 

Funding: DoE SBIR 2008 Phase II, DE-FG02-07ER84821


High frequency, high power rf sources are needed for many applications in particle accelerators, communications, radar, etc. We have developed a 26GHz high power rf source based on the extraction of wakefields from a relativistic electron beam. The extractor is designed to couple out rf power generated from a high charge electron bunch train traversing a dielectric loaded waveguide. Using a 20nC bunch train (bunch length of 1.5 mm) at the Argonne Wakefield Accelerator (AWA) facility, we expect to obtain a steady 26GHz output power of 148 MW. The extractor has been fabricated and bench tested along with a 26GHz Power detector. The first high power beam experiments should be performed prior to the Conference. Detailed results will be reported.

 
WE6RFP061 A Transverse Mode Damped DLA Structure vacuum, wakefield, damping, controls 2933
 
  • C.-J. Jing, F. Gao, A. Kanareykin, P. Schoessow
    Euclid TechLabs, LLC, Solon, Ohio
  • M.E. Conde, W. Gai, R. Konecny, J.G. Power
    ANL, Argonne
 
 

Funding: DoE SBIR Phase I 2008


As the dimensions of accelerating structures become smaller and beam intensities higher, the transverse wakefields driven by the beam become quite large with even a slight misalignment of the beam from the geometric axis. These deflection modes can cause inter-bunch beam breakup and intra-bunch head-tail instabilities along the beam path, and thus BBU control becomes a critical issue. All new metal based accelerating structures, like the accelerating structures developed at SLAC or power extractors at CLIC, have designs in which the transverse modes are heavily damped. Similarly, minimizing the transverse wakefield modes (here the HEMmn hybrid modes in Dielectric-Loaded Accelerating (DLA) structures) is also very critical for developing dielectric based high energy accelerators. We have developed a 7.8GHz transverse mode damped DLA structure. The design and bench test results are presented in the article.

 
WE6RFP063 Studies of Beam Breakup in Dielectric Structures wakefield, focusing, laser, pick-up 2939
 
  • A. Kanareykin, C.-J. Jing, A.L. Kustov, P. Schoessow
    Euclid TechLabs, LLC, Solon, Ohio
  • W. Gai, J.G. Power
    ANL, Argonne
 
 

Funding: This work is supported by the US Department of Energy


Beam breakup (BBU) effects resulting from parasitic wakefields provide a potentially serious limitation to the performance of dielectric structure based accelerators. We report here on comprehensive numerical studies and planned experimental investigations of BBU and its mitigation in dielectric wakefield accelerators. An experimental program is planned at the Argonne Wakefield Accelerator facility that will focus on BBU measurements in a number of high gradient and high transformer ratio wakefield devices. New pickup-based beam diagnostics will provide methods for studying parasitic wakefields that are currently unavailable at the AWA. The numerical part of this research is based on a particle-Green’s function beam dynamics code (BBU-3000) that we are developing. The code allows rapid, efficient simulation of beam breakup effects in advanced linear accelerators. The goal of this work is to compare the results of detailed experimental measurements with accurate numerical results and ultimately to study the use of external FODO channels for control of the beam in the presence of strong transverse wakefields.

 
WE6RFP064 Accelerator Applications of New Nonlinear Ferroelectric Materials wakefield, controls, acceleration, high-voltage 2942
 
  • P. Schoessow, A. Kanareykin
    Euclid TechLabs, LLC, Solon, Ohio
  • E.V. Kozyrev
    LETI, Saint-Petersburg
  • V.P. Yakovlev
    Fermilab, Batavia
 
 

Funding: Work supported by the US Department of Energy.


Materials possessing large variations in the permittivity as a function of the electric field exhibit a rich variety of phenomena for electromagnetic wave propagation such as frequency multiplication, wave steepening and shock formation, solitary waves, and mode mixing. New low loss nonlinear microwave ferroelectric materials present interesting and potentially useful applications for both advanced and conventional particle accelerators. Accelerating structures (either wakefield-based or driven by an external rf source) loaded with a nonlinear dielectric may exhibit significant field enhancements. Nonlinear transmission lines can be used to generate short, high intensity rf pulses to drive fast rf kickers. In this paper we will explore the large signal permittivity of these new materials and applications of nonlinear dielectric devices to high gradient acceleration, rf sources, and beam manipulation. We describe planned measurements using a planar nonlinear transmission line to study the electric field dependence of the permittivity of these materials. Diagnostics include appearance of harmonics with a cw drive signal and sharpening of a pulse waveform as it propagates.

 
WE6RFP071 Emission of Collimated X-Ray Radiation in Laser-Wakefield Experiments Using Particle Tracking in PIC Simulations radiation, electron, plasma, laser 2958
 
  • J.L. Martins, R.A. Fonseca, S.F. Martins, L.O. Silva
    Instituto Superior Tecnico, Lisbon
  • C. Joshi, W.B. Mori
    UCLA, Los Angeles, California
 
 

Funding: F.C.Gulbenkian, F.C.T. [SFRH/BD/35749/2007, SFRH/BD/39523/2007, PTDC/FIS/66823/2006 (Portugal)], and European Community (project EuroLeap, contract #028514)


It is now accepted that self-trapped electrons in a laser wakefield accelerator operating in the "bubble" regime undergo strong periodic oscillations about the wakefield axis because of the focusing force provided by the ions. This betatron motion of the off-axis electrons results in the emission of x-ray radiation strongly peaked in the forward direction. Even though the x-rays are broadband with a synchrotron-like spectrum, their brightness can be quite high because of their short pulse duration and strong collimation. We employ particle tracking in particle in cell simulations with OSIRIS*, combined with a post-processing radiation diagnostic, to evaluate the features of the radiation mechanisms of accelerated electrons in LWFA experiments. We show and discuss results for a 1.5 GeV laser wakefield accelerator stage. A study of the angular dependence of the radiated power is also presented and compared with theoretical models. This analysis also allows for the direct calculation of the radiation losses of the self-injected bunch.


*R. A. Fonseca et al, LNCS 2329, III-342, Springer-Verlag, (2002)

 
WE6RFP073 Controlled Injection in the Sharp Phase Mixing Region of LWFA electron, laser, plasma, injection 2964
 
  • S.H. Yoo, J. Kim, J.-U. Kim
    KERI, Changwon
 
 

Funding: Korea Electrotechnology Research Institute (KERI)


To generate the good quality electron bunch, stable fast injection is very important issue in the laser wakefield accelerator(LWFA). One of the self-injection methods is the wave breaking*. In this scheme, the density transition scale length is much larger than plasma skin depth. After a new self-injection mechanism using the sharp density transition scheme was proposed**, the experiment for the generation of the plasma shock structure have been conducted***. In this scheme, while one can reduce the wave breaking, the electron can be injected effectively using a phase mixing. Thus, the sharp density transition scheme is promising candidate method for the more stable generation of good quality electron bunch. In this scheme, the main issue is that the finding optimum conditions in which the injected electrons only in the first period of laser wake wave are accelerated further. In this paper, optimum conditions of sharp density transition scheme have been studied using Particle-In-Cell simulations. And the transverse parabolic profile is used to increase the beam quality. Throughout the extensive simulation work, the optimum conditions for the experiments at KERI is presented.


*S. Bulanov, et. al., Phys. Rev. E, 58, R5257 (1998)
**H. Suk, et. al., Phys. Rev. Lett. 86, {10}11 (2001)
***J. U. Kim, et. al., 69, 026409 (2004)

 
WE6RFP075 Scaled Simulation Design of High Quality Laser Wakefield Accelerator Stages laser, plasma, focusing, electron 2970
 
  • C.G.R. Geddes, E. Cormier-Michel, E. Esarey, W. Leemans, C.B. Schroeder
    LBNL, Berkeley, California
  • D.L. Bruhwiler, J.R. Cary, B.M. Cowan, C. Nieter, K. Paul
    Tech-X, Boulder, Colorado
 
 

Funding: Funded by the U.S. DOE Office of Science HEP including contract DE-AC02-05CH11231 and SciDAC, and by U.S. DOE NA-22, DARPA, and NSF


Collider and light source applications of laser wakefield accelerators will likely require staging of controlled injection with multi-GeV accelerator modules to produce and maintain the required low emittance and energy spread. We present simulations of upcoming 10 GeV-class LWFA stages, towards eventual collider modules for both electrons and positrons*.  Laser and structure propagation are controlled through a combination of laser channeling and self guiding.  Electron beam evolution is controlled through laser pulse and plasma density shaping, and beam loading. This can result in efficient stages which preserve high quality beams.  We also present results on controlled injection of electrons into the structure to produce the required low emittance bunches using plasma density gradient** and colliding laser pulses.  Tools for accurately modeling emittance and energy spread will be discussed***.


*E. Cormier-Michel et al., Proc. Adv Accel. Workshop 2008.
**C.G.R. Geddes et al., PRL 2008.
***E. Cormier-Michel et al, PRE 2008; C.G.R. Geddes et al, Proc. Adv Accel. Workshop 2008.

 
WE6RFP081 Design of Advanced Photonic Bandgap (PBG) Structures for High Gradient Accelerator Applications damping, dipole, HOM, wakefield 2986
 
  • R.A. Marsh, B.J. Munroe, M.A. Shapiro, R.J. Temkin
    MIT/PSFC, Cambridge, Massachusetts
 
 

Funding: Work supported by DOE HEP, under contract DE-FG02-91ER40648


The design of advanced photonic bandgap (PBG) accelerator structures is examined. PBG structures are chosen for their wakefield damping. A potential disadvantage of PBG structures, as well as damped detuned structures, is the increased wall currents at the structure surface due to the reduced surface area, leading to higher pulsed wall heating. Research is carried out to improve the pulsed heating performance of PBG structure concepts while maintaining higher order mode damping. Wakefield damping parameters are discussed and a quantitative figure of merit is expressed to evaluate and compare PBG concepts. Pulsed heating performance in PBG structures is improved by breaking perfect symmetry and allowing deformation of both rod and lattice geometry. A final design for an improved pulsed heating performance PBG structure for breakdown testing at 11.424 GHz is presented and discussed.

 
WE6RFP082 Design of Photonic Bandgap (PBG) Accelerator Structures with Reduced Symmetry dipole, damping, HOM, wakefield 2989
 
  • B.J. Munroe, R.A. Marsh, M.A. Shapiro, R.J. Temkin
    MIT/PSFC, Cambridge, Massachusetts
 
 

Funding: Work supported by DOE HEP, under contract DE-FG02-91ER40648


The design of a new photonic bandgap (PBG) accelerator structure based on a pentagonal array of rods is presented. The goal of this structure is to damp the higher order modes (HOMs) present in the structure. By removing the bilateral symmetry present in the four and six rod PBG structures the five rod photonic quasi-crystal (PQC) structure is able to damp the symmetric dipole mode. The field pattern and mode Q factors for the fundamental and dipole modes are presented for various values of the ratio of rod radius to rod spacing. These results are compared to the equivalent results for the six rod structure. The ratio of the Q factors is also calculated, and found to show an optimal value near a rod radius to rod spacing ratio of 0.17 in both cases.

 
WE6RFP083 Metamaterial-Based Linear Accelerator Structure electron, acceleration, coupling, impedance 2992
 
  • M.A. Shapiro, J.R. Sirigiri, R.J. Temkin
    MIT/PSFC, Cambridge, Massachusetts
  • G. Shvets
    The University of Texas at Austin, Austin, Texas
 
 

Funding: US Department of Energy, Office of High Energy Physics


Negative refraction metamaterials (NR MTL) have been developed at microwave, THz, and optical frequencies. At present, microwave MTL's are studied for applications such as microwave filters and patch antennas. Accelerator-relevant applications, such as measuring electron bunch length using its inverse Cherenkov radiation in a NR MTL, have also been proposed. Here we propose a MTL based linear accelerator structure. The MTL is built as an array of complimentary split-ring resonators cut in two metallic plates. The accelerating electron bunch traverses between the plates. The operating mode's properties and standard accelerator parameters (R/Q, accelerating gradient, etc.) of the proposed structure will be reported.

 
WE6RFP086 Analytical and Numerical Investigation of a Coaxial Two-Channel Dielectric Wakefield Accelerator wakefield, electron, acceleration, focusing 2998
 
  • G.V. Sotnikov
    NSC/KIPT, Kharkov
  • J.L. Hirshfield
    Yale University, Physics Department, New Haven, CT
  • T.C. Marshall, G.V. Sotnikov
    Omega-P, Inc., New Haven, Connecticut
  • S.V. Shchelkunov
    Yale University, Beam Physics Laboratory, New Haven, Connecticut
 
 

Funding: The research was supported by US Department of Energy, Office of High Energy Physics, Advanced Accelerator R & D.


A new scheme for a dielectric wakefield accelerator is proposed that em-ploys a cylindrical multi-zone dielectric structure configured as two concentric dielectric tubes with outer and inner vacuum channels for drive and accelerated bunches. Analytical and numerical studies have been carried out for such coaxial dielectric-loaded structures (CDS) for high-gradient acceleration. An analytical theory of wakefield excitation by particle bunches in a multi-zone CDS has been formulated. Numerical calculations were made for an example of a CDS using dielectric tubes of material with dielectric permittivity 5.7, having external diameters of 2.121 mm and 0.179 mm with inner diameters of 2.095 mm and 0.1 mm. An annular 5 GeV, 5 nC electron bunch with RMS length of 0.14 mm energizes a wakefield on the structure axis having an accelerating gradient of ~600 MeV/m with a transformer ratio ~8. The period of the accelerating field is ~0.38 mm. Full numerical simulation using a PIC code has confirmed results of the linear theory and furthermore has shown the important influence of the quenching wave. The simulation also has shown stable transport of drive and accelerated bunches through the CDS.

 
WE6RFP090 Woodpile Structure Fabrication for Photonic Crystal Laser Acceleration laser, acceleration, alignment, electron 3008
 
  • C. McGuinness
    SLAC, Menlo Park, California
 
 

We present recent progress in the fabrication of a 3D photonic crystal laser accelerator structure. Direct acceleration of electrons by lasers offer promising improvements over traditional RF acceleration techniques in terms of cost, gradient, technology used, and short temporal bunches produced. Microbunching and net acceleration experiments were successfully performed at the E163 facility at SLAC, setting the stage for design, fabrication, and testing of optical structures. This paper describes work done at the Stanford Nanofabrication Facility towards fabricating such structures. A process based on standard optical lithographic techniques was used to fabricate a four layer woodpile photonic crystal with a bandgap centered at 4.55μm and a full width half max of 2.71μm. Infrared spectroscopy measurements were taken and compared with simulations yielding good agreement. SEM images were used to measure fabrication deviations in rod width, rod shape, layer thickness, and alignment, and further simulations are being done to study the effect of these deviations on properties of the accelerating mode excited in the defect of a 20 layer structure currently under design.

 
WE6RFP092 Axial Channeling of Positively Charged High-Energy Proton Beams proton, scattering, alignment, lattice 3010
 
  • V. Guidi, S. Baricordi, P. Dalpiaz, M. Fiorini
    UNIFE, Ferrara
  • A.G. Afonin, Y.A. Chesnokov, V.A. Maisheev, I.A. Yazynin
    IHEP Protvino, Protvino, Moscow Region
  • G. Ambrosi, B. Bertucci, W.J. Burger, P. Zuccon
    INFN-PG, Perugia
  • D. Bolognini, S. Hasan, A. Mozzanica, M. Prest
    Università dell'Insubria & INFN Milano Bicocca, Como
  • G. Cavoto, R. Santacesaria, P. Valente
    INFN-Roma, Roma
  • G. Della Mea, R. Milan, A. Vomiero
    INFN/LNL, Legnaro (PD)
  • A.S. Denisov, Yu.A. Gavrikov, Yu.M. Ivanov, L.P. Lapina, L.G. Malyarenko, V. Skorobogatov, V.M. Suvorov, S.A. Vavilov
    PNPI, Gatchina, Leningrad District
  • A.D. Kovalenko, A.M. Taratin
    JINR, Dubna, Moscow Region
  • C. Luci
    Università di Roma I La Sapienza, Roma
  • A. Mazzolari
    INFN-Ferrara, Ferrara
  • W. Scandale
    CERN, Geneva
  • E. Vallazza
    INFN-Trieste, Trieste
 
 

The H8RD22 collaboration has accomplished an extensive study of axial channeling in the external lines of the CERN SPS. For 400 GeV protons, it was recorded deflection by about 90% of the particles by a short crystal, by far exceeding the performance of previous experiments. Axial channeling with 150 GeV negative hadrons was also firmly observed with deflection capability comparable to the case of positive particles. Near-axis effect such as multiple-volume reflections in a single crystal as a result of the superposition of volume reflections by a series of parallel planes sharing the same axis was investigated with 400 GeV protons. Confirmation of theoretical expectation was observed, in particular most of the particles were deflected by about 50 urad, four times the deflection angle imparted by a single volume reflection of most efficient planes. In this case the angular acceptance was sensitively broader than for the case of channeling. In summary, channeling in axial mode and multi-volume reflections were proven to be two mechanisms for manipulation steering of high-energy particle beams, which side most established techniques such as planar channeling and volume reflection.*


*Contribution on behalf of the H8RD22 collaboration.

 
WE6RFP097 Simulations of 25 GeV PWFA Sections: Path Towards a PWFA Linear Collider plasma, acceleration, collider, electron 3025
 
  • C. Huang, W. An, C.E. Clayton, C. Joshi, W. Lu, K.A. Marsh, W.B. Mori, M. Tzoufras
    UCLA, Los Angeles, California
  • I. Blumenfeld, M.J. Hogan, N.A. Kirby, T.O. Raubenheimer, A. Seryi
    SLAC, Menlo Park, California
  • T.C. Katsouleas
    Duke University, Durham, North Carolina
  • P. Muggli
    USC, Los Angeles, California
 
 

Funding: Work supported by DOE under contracts DE-FG03-92ER40727, DE-FG52-06NA26195, DE-FC02-07ER41500, DE-FG02-03ER54721.


Recent Plasma Wake-Field Acceleration (PWFA) experiments at Stanford Linear Accelerator Center has demonstrated electron acceleration from 42GeV to 84GeV in less than one meter long plasma section. The accelerating gradient is above 50GeV/m, which is three orders of magnitude higher than those in current state-of-art RF linac. Further experiments are also planned with the goal of achieving acceleration of a witness bunch with high efficiency and good quality. Such PWFA sections with 25 GeV energy gain will be the building blocks for a staged TeV electron-positron linear collider concept based on PWFA (PWFA-LC). We conduct Particle-In-Cell simulations of these PWFA sections at both the initial and final witness beam energies. Different design options, such as Gaussian and shaped bunch profiles, self-ionized and pre-ionized plasmas, optimal bunch separation and plasma density are explored. Theoretical analysis of the beam-loading* in the blow-out regime of PWFA and simulation results show that highly efficient PWFA stages are possible. The simulation needs, code developments and preliminary simulation results for future collider parameters will be discussed.


*M. Tzoufras et al, Phys. Rev. Lett. {10}1, 145002 (2008).

 
WE6RFP098 High Transformer Ratio PWFA for Application on XFELs plasma, electron, wakefield, emittance 3028
 
  • W. Lu, W. An, C. Huang, C. Joshi, W.B. Mori
    UCLA, Los Angeles, California
  • M.J. Hogan, T.O. Raubenheimer, A. Seryi
    SLAC, Menlo Park, California
 
 

Funding: Work supported by DOE grant numbers: DE-FG03-92ER40727, DE-FG52-06NA26195, DE-FC02-07ER41500, DE-FG02-03ER54721


The fourth generation of light sources (such as LCLS and the XFEL) require high energy electron drivers (16-20GeV) of very high quality. We are exploring the possibility of using a high transformer ratio PWFA to meet these challenging requirements. This may have the potential to reduce the size of the electron drivers by a factor of 5 or more, therefore making these light source much smaller and more affordable. In our design, a high charge (5-10nC) low energy driver (1-3GeV) with an elongated current profile is used to drive a plasma wake in the blowout regime with a high transformer ratio (5 or more). A second ultra-short beam that has high quality and low charge beam (1nC) can be loaded into the wake at a proper phase and be accelerated to high energy (5-15GeV) in very short distances (10s of cms). The parameters can be optimized, such that high quality (0.1% energy spread and 1mm mrad normalized emittance) and high efficiency (60-80%) can be simultaneously achieved. The major obstacle for achieving the above goals is the electron hosing instabilities in the blowout regime. In this poster, we will use both theoretical analysis and PIC simulations to study this concept.

 
WE6RFP099 Investigation of Ionization Induced Trapping in a Laser Wakefield Accelerator laser, electron, plasma, wakefield 3031
 
  • A.E. Pak, C. Joshi, K.A. Marsh, W.B. Mori
    UCLA, Los Angeles, California
  • S.F. Martins
    Instituto Superior Tecnico, Lisbon
 
 

Funding: Work Supported by DOE Grant DEFG02-92ER40727


Controlling the trapping of electrons into accelerating wakefields is an important step to obtaining a stable reproducible electron beam from a laser wakefield accelerator (LWFA). Recent experiments at UCLA have focused on using the different ionization potentials of gases as a mechanism for controlling the trapping of electrons into an LWFA. The accelerating wakefield was produced using an ultra-intense (Io ~ 1019 W / cm2 ), ultra-short (τFWHM ~ 40 fs) laser pulses. The laser pulse was focused onto the edge of column of gas created by a gas jet. The gas was a mixture of helium and nitrogen. The rising edge of the laser pulse fully ionizes the helium and the first five bound electrons of the nitrogen. Only at the peak of the laser pulse is it intense enough to ionize the most tightly bound electrons of the nitrogen. Electrons which are ionized at the peak of laser pulse are born into a favorable phase space within the accelerating wakefield and are subsequently trapped and accelerated. The accelerated electrons were dispersed using a dipole magnet with a ~ 1 Tesla magnetic field onto a phosphor screen. Electron beam energy spectrum charge and divergence were measured.

 
WE6RFP102 Progress towards a 9.37GHz Hybrid Dielectric-Iris-Loaded Structure Filled with Low Loss Dielectric cavity, coupling, impedance, ion 3038
 
  • X.D. He, S. Dong, Y.J. Pei, C.-F. Wu
    USTC/NSRL, Hefei, Anhui
 
 

Funding: the National Nature Science Foundation of China, Grant No. 10375060, 10375061 and 10675116


One of the major concerns in the development of hybrid dielectric-iris-loaded structure is the performance of the used dielectric. The previous dielectric is machinable but the loss tangent is slightly high. So we adopt the new dielectric (Mg-Ca-Ti-O) with loss tangent of about 2·10-4. Because of its high hardness and brittleness, the machining technology and methods are attempted. In this paper, we present a new design of the structure. The model cavities and the coupler for this structure with the new dielectric are investigated experimentally. The experiment results are accorded with the simulated results. In the end, the amplitude and phase shift of the electric field and R/Q of this structure at the operation frequency are even got by a bead-pull experiment.

 
WE6RFP103 Development of X-band Photonic Band Gap Accelerating Structure cavity, coupling, HOM, damping 3041
 
  • Z.P. Li
    USTC, Hefei, Anhui
  • S. Dong, X.D. He, C.-F. Wu
    USTC/NSRL, Hefei, Anhui
 
 

Funding: National Nature Science Foundation of China, Grant No. 10675116 and 10375060


We present the new experimental results for an X-band (11.42GHz) metallic PBG accelerating cavity. A coupler of a single cavity was fabricated and cold tested. An X-band traveling-wave PBG accelerator was designed based on CST MWS transient analysis. The X-band PBG accelerator is now under construction, future work will focus on the structure to be cold tested and tuned.

 
TH3GAI01 Electron Beam Dynamics in the Long-Pulse, High-Current DARHT-II Linear Induction Accelerator electron, dipole, induction, solenoid 3080
 
  • C. Ekdahl, E.O. Abeyta, P. Aragon, R.D. Archuleta, G.V. Cook, D. Dalmas, K. Esquibel, R.J. Gallegos, R.W. Garnett, J.F. Harrison, E.B. Jacquez, J.B. Johnson, B.T. McCuistian, N. Montoya, S. Nath, K. Nielsen, D. Oro, L.J. Rowton, M. Sanchez, R.D. Scarpetti, M. Schauer, G.J. Seitz, H.V. Smith, R. Temple
    LANL, Los Alamos, New Mexico
  • R. Anaya, G.J. Caporaso, F.W. Chambers, Y.-J. Chen, S. Falabella, G. Guethlein, B.A. Raymond, R.A. Richardson, J.A. Watson, J.T. Weir
    LLNL, Livermore, California
  • H. Bender, W. Broste, C. Carlson, D. Frayer, D. Johnson, C.-Y. Tom, C.P. Trainham, J.T. Williams
    NSTec, Los Alamos, New Mexico
  • T.C. Genoni, T.P. Hughes, C.H. Thoma
    Voss Scientific, Albuquerque, New Mexico
  • B.A. Prichard, M.E. Schulze
    SAIC, Los Alamos, New Mexico
 
 

Funding: This work was supported by the US National Nuclear Security Agency and the US Department of Energy under contract W-7405-ENG-36.


The DARHT-II linear induction accelerator (LIA) now accelerates 2-kA electron beams to more than 17 MeV. This LIA is unique in that the accelerated current pulse width is greater than 2 microseconds. This pulse has a flat-top region where the final electron kinetic energy varies by less than 1% for more than 1.5 microseconds. The long risetime of the 6-cell injector current pulse is 0.5 microsecond, which can be scraped off in a beam-head cleanup zone (BCUZ) before entering the 68-cell main accelerator. We discuss our experience with tuning this novel accelerator; and we will present data for the resulting beam transport and dynamics. We will also present beam stability data, and relate these to previous stability experiments at lower current and energy*.


* “Long-pulse beam stability experiments on the DARHT-II linear induction accelerator,” Carl Ekdahl, et al., IEEE Trans. Plasma. Sci. Vol. 34, 2006, pp. 460-466

 

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TH3GAI04 Progress in Beam Focusing and Compression for Target Heating and Warm Dense Matter Experiments plasma, target, solenoid, ion 3095
 
  • P.A. Seidl, A. Anders, F.M. Bieniosek, J.E. Coleman, J.-Y. Jung, M. Leitner, S.M. Lidia, B.G. Logan, P.N. Ni, D. Ogata, P.K. Roy, W.L. Waldron
    LBNL, Berkeley, California
  • J.J. Barnard, R.H. Cohen, D.P. Grote
    LLNL, Livermore, California
  • M. Dorf, E.P. Gilson
    PPPL, Princeton, New Jersey
  • D.R. Welch
    Voss Scientific, Albuquerque, New Mexico
 
 

The Heavy-Ion Fusion Sciences Virtual National Laboratory is pursuing an approach to target heating experiments in the warm dense matter regime, using space-charge-dominated ion beams that are simultaneously longitudinally bunched and transversely focused. Longitudinal beam compression by large factors has been demonstrated in the Neutralized Drift Compression Experiment (NDCX) with controlled ramps and forced neutralization. Using an injected 30 mA K+ ion beam with initial kinetic energy 0.3 MeV, axial compression leading to ~100X current amplification and simultaneous radial focusing to a few mm have led to encouraging energy deposition approaching the intensities required for eV-range target heating experiments. We discuss the status of several improvements to NDCX to reach the necessary higher beam intensities, including:

  1. greater axial compression via a longer velocity ramp;
  2. beam steering dipoles to mitigate aberrations in the bunching module;
  3. time-dependent focusing elements to correct considerable chromatic aberrations; and
  4. plasma injection improvements to establish a plasma density always greater than the beam density, expected to be >1013 cm-3.

 

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TH3GBI04 Generation of Bunch Trains for Plasma Wakefield Accelerator Applications plasma, emittance, focusing, wakefield 3110
 
  • P. Muggli
    USC, Los Angeles, California
 
 

Funding: Work supported by US Department of Energy


Preservation of the incoming beam emittance is a key characteristic needed for any accelerating system, including the beam-driven, plasma-based accelerator or plasma wakefield accelerator (PWFA). Electron beams with a density larger than the plasma density propagate in a pure and uniform plasma ion column that acts as a focusing element free of geometric aberrations, and the beam emittance is preserved. On the contrary, positron beams attract plasma electrons that flow through the beam and create a non-uniform charge density inside the beam that can exceed the beam density. The resulting plasma focusing force is non-uniform and non-linear. Experimentally, we observe the formation of a beam halo on a screen placed downstream from the plasma. Analysis of the beam images as a function of the plasma density show that the transverse beam size at the screen is strongly reduced in the high emittance plane, and that in the low emittance plane charge is transferred from the beam core to the halo. Numerical simulations of the experiments show the same behavior and indicate that there is emittance growth is both planes. Experimental and simulations will be presented.

 

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TH4GBC05 Boosted Frame PIC Simulations of LWFA: Towards the Energy Frontier plasma, laser, electron, radiation 3160
 
  • S.F. Martins, R.A. Fonseca, L.O. Silva
    Instituto Superior Tecnico, Lisbon
  • W. Lu, W.B. Mori
    UCLA, Los Angeles, California
 
 

Funding: F.C.Gulbenkian, F.C.T. [SFRH/BD/35749/2007, PTDC/FIS/66823/2006 (Portugal)], and European Community - New and Emerging Science and Technology Activity, FP6 program (project EuroLeap, contract #028514)


We address full particle-in-cell simulations of the next generation of Laser Wakefield Accelerators with energy gains > 10 GeV. The distances involved in these numerical experiments are very demanding in terms of computational resources and are not yet possible to (easily) accomplish. Following the work on simulations of particle beam-plasma interaction scenarios in optimized Lorentz frames by J.-L. Vay*, the Lorentz transformation for a boosted frame was implemented in OSIRIS**, leading to a dramatic change in the computational resources required to model LWFA. The critical implementation details will be presented, and the main difficulties discussed. Quantitative comparisons between lab/boost frame results with OSIRIS, QuickPIC***, and experiment will be given. Finally, the results of a three-dimensional PIC simulation of a > 10 GeV accelerator stage will be presented, including a discussion on radiation emission.


* J.-L. Vay, PRL 98, 130405 (2007)
** R.A. Fonseca et al., LNCS 2329, III-342 (Springer-Verlag, 2002)
*** C. Huang, et al., JCP 217, Issue 2, 20 (2006)

 

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Slides

 
TH4PBC04 Emittance Degradation of Sources due to Utilization of Transverse RF Deflectors in Taiwan Photon Source emittance, electron, sextupole, cavity 3175
 
  • H. Ghasem, G.-H. Luo
    NSRRC, Hsinchu
 
 

Since use of such deflecting structures leads to growth in vertical amplitude and slope of electrons, non-zero momentum compaction factor, nonlinearities and coupling of the elements between the deflectors affect the tilted electrons even in perfect machine and change their amplitude and slope at second deflecting cavity. It causes the second deflector cannot cancel the first kick perfectly and leads to increase of transverse emittance. We have studied simulation and detail analyses of effects of non-zero momentum compaction factor and sextupoles between the deflecting structures, as sources of emittance degradation in TPS and evaluate how much emittance growths due to the effects. We also contrast the statuses of interior sextupoles and elucidate them.

 
TH5PFP001 Large Scale Simulations of the Fermilab 8-GeV H-Minus Linac: Beam Loss Studies from Machine Errors and H- Stripping linac, beam-losses, H-minus, emittance 3184
 
  • B. Mustapha, P.N. Ostroumov, J. Xu
    ANL, Argonne
  • J.-P. Carneiro
    Fermilab, Batavia
 
 

Funding: This work was supported by the U.S. Department of Energy, Office of Nuclear Physics, under Contract No. DE-AC02-06CH11357.


The latest version of PTRACK*, the parallel version of the beam dynamics code TRACK, is capable of simulating a very large number of particles (a billion or more). In the case of the Fermilab 8-GeV H-minus linac, it is possible to simulate the actual number of particles in the bunch. Taking advantage of this capability we are revisiting our original beam loss studies**, but this time with larger statistics and including a new process of beam loss which is the stripping of H- ions. TRACK has recently been updated*** with the possibility of stripping H- by three different processes, namely black body radiation, Lorentz force stripping and residual gas interactions. Results of ideal end-to-end simulations (no errors) with the actual number of particles in a beam bunch (860M) as well as error simulations for different sets of errors with 10M and eventually 100M particles per seed will be presented and discussed. These simulations are being performed on Argonne's new petascale computing facility "BG/P".


* J. Xu et al, Proceedings of HB-2008.
** P. Ostroumov, B. Mustapha and V.A. Aseev, Proceedings of Linac-06.
*** J.-P. Carneiro, B. Mustapha and P. Ostroumov, submitted to PRST-AB.

 
TH5PFP002 Simulation of Electron Cloud Density Distributions in RHIC Dipoles at Injection and Transition and Estimates for Scrubbing Times electron, injection, dipole, proton 3187
 
  • P. He, M. Blaskiewicz, W. Fischer
    BNL, Upton, Long Island, New York
 
 

In this report we summarize electron-cloud simulations for the RHIC dipole regions at injection and transition to estimate if scrubbing at injection would reduce the electron cloud density at transition. We simulate the horizontal electron cloud distribution in the RHIC dipoles for secondary electron yields (SEY) from 1.1 to 2.0 at injection (with a bunch intensity of 1.3x109) and at transition (with a bunch intensity of 1.2x109). Also, we unveil the sensitivity to rather small changes in bunch intensity from 1.0 x109 to 1.5x109 , when SEY keep at 1.4 and 1.5 both for injection and transition.

 
TH5PFP004 Final Design of the IFMIF-EVEDA Low Energy Beam Transport Line rfq, injection, space-charge, solenoid 3190
 
  • N. Chauvin, O. Delferrière, R.D. Duperrier, R. Gobin, P.A.P. Nghiem, D. Uriot
    CEA, Gif-sur-Yvette
  • M. Comunian
    INFN/LNL, Legnaro (PD)
 
 

During the EVEDA (Engineering Validation and Engineering Design Activities) phase of the IFMIF (International Fusion Materials Irradiation Facility) project, a 125 mA/9 MeV accelerator prototype will be built, tested and operated in Rokkasho-Mura (Japan). The injector section of this accelerator is composed by an ECR source, delivering a 140 mA deuteron beam at 100 keV, and a low energy beam transport (LEBT) line required to match the beam for the RFQ injection. The proposed design for the LEBT is based on a dual solenoids focusing scheme. In order to takes into account the space charge compensation of the beam induced by the ionisation of the residual gas, a 3D particle-in-cell code (SOLMAXP) has been developed for the beam dynamics calculations. The LEBT parameters have been optimized in order to maximize the beam transmission through the RFQ. The final LEBT design, as well as the simulation results, are presented.

 
TH5PFP005 Optimization Results of Beam Dynamics Simulations for the Superconducting HWR IFMIF Linac linac, solenoid, cryomodule, quadrupole 3193
 
  • N. Chauvin, R.D. Duperrier, A. Mosnier, P.A.P. Nghiem, D. Uriot
    CEA, Gif-sur-Yvette
 
 

The 250 mA, 40 MeV cw deuteron beam required for the International Fusion Materials Irradiation Facility (IFMIF) will be provided by two 125 mA linacs. In order to accelerate the beam from 5 MeV to 40 MeV, a superconducting linac, housed in four cryomodules, is proposed. The design is based on two beta families (beta=0.094 and beta=0.166) of half-wave resonators (HWR) at 175 MHz. The transverse focusing is achieved using one solenoid coil per lattice. This paper presents the extensive multi-particle beam dynamics simulations that have been performed to adapt the beam along the SC-HWR structure in such a high space charge regime. As one of the constraints of the IFMIF linac is hands-on maintenance, specific optimizations have been done to minimize the beam occupancy in the line (halo). A Monte Carlo error analysis has also been carried out to study the effects of misalignments or field imperfections.

 
TH5PFP008 Accelerator Physics Concept for Upgraded LHC Collimation Performance collimation, impedance, ion, proton 3202
 
  • R.W. Assmann, G. Bellodi, J.M. Jowett, E. Métral, Th. Weiler
    CERN, Geneva
  • L. Keller, T.W. Markiewicz
    SLAC, Menlo Park, California
 
 

The LHC collimation system is implemented in phases, in view of the required extrapolation by 2-3 orders of magnitude beyond Tevatron and HERA experience in stored energy. All available simulations predict that the LHC proton beam intensity with the "phase 1" collimation system may be limited by the impedance of the collimators or cleaning efficiency. Maximum efficiency requires collimator materials very close to the beam, generating the dominant resistive impedance in the LHC. Above a certain intensity the beam is unstable. On the other hand, even if collimators are set very close to the beam, the achievable cleaning efficiency is predicted to be inadequate, requiring either beam stability beyond specifications or reduced intensity. The accelerator physics concept for upgrading cleaning efficiency, for both proton and heavy ion beams, and reducing collimator-related impedance is described. Besides the "phase 2" secondary collimators, new collimators are required in a few super-conducting regions.

 
TH5PFP011 Simulation of Beam-Gas Scattering in the LHC proton, scattering, background, collimation 3208
 
  • Y.I. Levinsen, H. Burkhardt
    CERN, Geneva
  • V. Talanov
    IHEP Protvino, Protvino, Moscow Region
 
 

We report on background studies for the LHC with detailed simulations. The simulations now include generation of beam-gas scattering in combination with multiturn tracking of protons. Low beta optics and available aperture files for this configuration have been used to generate loss maps according to the pressure distribution in the LHC.

 
TH5PFP016 Tune Shift due to Crossing Collision and Crab Collision cavity, luminosity, quadrupole, resonance 3223
 
  • Y. Sun, R. Tomás, F. Zimmermann
    CERN, Geneva
 
 

Funding: This work was supported by the European Community-Research Infrastructure Activity under the FP6 "Structuring the European Research Area" programme (CARE, contract number RII3-CT-2003-506395).


The use of crab cavities in the LHC may not only raise the luminosity, but it could also complicate the beam dynamics, e.g. crab cavities might not only cancel synchro-betatron resonances excited by the crossing angle but they could also excite new ones. In this paper, we use weak-strong beam-beam model to study the incoherent linear tune shift of the weak beam, for the crossing collision case and crab collision case with a finite crossing angle. The tune shift is also compared among the head-on collision, crossing collision and crab collision cases, both analytically and numerically.

 
TH5PFP017 Space Charge Simulations for the Mu2e Experiment at Fermilab space-charge, antiproton, extraction, proton 3226
 
  • J.F. Amundson, P. Spentzouris, E.G. Stern
    Fermilab, Batavia
 
 

The proposed Mu2e experiment will present a number of challenges for the Fermilab accelerator complex. The Accumulator and Debuncher rings of what is currently the antiproton complex will be required to handle proton beams with intensities several orders of magnitude larger than the antiproton beams they now carry, leading to a substantial space-charge tune shift. The protons will be then be extracted from the Debuncher using resonant extraction. We present results from simulations of 3D space charge effects for Mu2e beam parameters, with emphasis on how they affect the resonant extraction process.

 
TH5PFP018 Recent Advances in the Synergia Accelerator Simulation Framework space-charge, impedance, optics, dipole 3227
 
  • J.F. Amundson, A. Macridin, P. Spentzouris, E.G. Stern
    Fermilab, Batavia
 
 

The Synergia framework has been enhanced to include new Poisson solvers and new collective physics effects. Synergia now includes Sphyraena, a solver suite that provides the ability to handle elliptical beam pipes. Resistive wall effects, including intra- and inter-bunch effects in the presence of multiple bunches are also available. We present an overview of the updates in Synergia, focusing on these developments.

 
TH5PFP019 Microwave Transmission through the Electron Cloud at the Fermilab Main Injector: Simulation and Comparison with Experiment electron, proton, dipole, plasma 3230
 
  • P. Lebrun
    Fermilab, Batavia
  • P. Stoltz, S.A. Veitzer
    Tech-X, Boulder, Colorado
 
 

Simulation of the microwave transmission properties through the electron cloud at the Fermilab Main Injector have been implemented using the plasma simulation code ‘‘VORPAL". Phase shifts and attenuation curves have been calculated for the lowest frequency TE mode, slightly above the cutoff frequency, in field free regions, in the dipoles and quadrupoles. Preliminary comparisons with experimental results are discussed and will guide the next generation of experiments.

 
TH5PFP021 RF Barrier Compression with Space Charge for the FAIR Synchrotrons space-charge, synchrotron, extraction, ion 3236
 
  • O. Boine-Frankenheim, O. Chorniy
    GSI, Darmstadt
 
 

The conservation of the longitudinal beam quality through the SIS-18/100 synchrotron chain is of major importance for the FAIR accelerator project as well as for the SIS-18 upgrade. The generation of a short, intense heavy ion bunch at the end of the machine cycle defines a tight budget for the tolerable longitudinal emittance growth. Potential sources of bunch quality degradation are intensity effects and non-adiabatic rf ramps during the rf capture in SIS-18 and during the barrier bucket pre-compression in SIS-100. The time spend on rf manipulations has to be as small as possible in order to maximize the repetition rate. We report about theoretical and experimental studies in SIS-18 of optimized voltage ramps for rf capture into single and double rf buckets, including space charge and beam-loading effects. Further we show that longitudinal space charge can improve the efficiency of rf manipulations. As an example we present an optimized barrier bucket pre-compression scheme for SIS-100.

 
TH5PFP023 High Intensity Nonlinear Dynamics in SIS100 beam-losses, space-charge, emittance, resonance 3242
 
  • G. Franchetti, I. Hofmann, S. Sorge
    GSI, Darmstadt
  • V.V. Kapin
    MEPhI, Moscow
 
 

Beam loss control in SIS100 is relevant for the design of collimators and for maintaining vacuum quality. We present the status of the studies of beam degradation, due to space charge and magnet imperfections during the accumulation at injection energy. The impact of magnet misalignment on resonances and beam trapping/scattering effects is discussed.

 
TH5PFP028 Longitudinal Particle Simulation for J-PARC RCS injection, extraction, acceleration, bunching 3254
 
  • M. Yamamoto, K. Hasegawa, M. Nomura, A. Schnase, T. Shimada, H. Suzuki, F. Tamura
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  • E. Ezura, K. Hara, C. Ohmori, M. Tada, A. Takagi, M. Yoshii
    KEK, Ibaraki
  • K. Horino
    Nippon Advanced Technology Co. Ltd., Ibaraki-prefecture
 
 

J-PARC RCS is in the beam commissioning period. Some longitudinal beam gymnastics and the acceleration has been successfully perfomed under the high intensity operation. We have developed a longitudinal particle tracking code, which includes beam loading and space charge effects. The comparison between the beam test result and the particle tracking simulation is described.

 
TH5PFP032 Status of Electron-Cloud Build-Up Simulations for the Main Injector dipole, electron, proton, injection 3266
 
  • M.A. Furman
    LBNL, Berkeley, California
  • I. Kourbanis, R.M. Zwaska
    Fermilab, Batavia
 
 

Funding: Supported by the US DOE under contract DE-AC02-05CH11231 and by the Fermilab Main Injector upgrade effort.


We provide a brief status report on measurements and simulations of the electron-cloud in the Fermilab Main Injector. Areas of agreement and disagreement are spelled out, along with their possible significance.

 
TH5PFP035 Space Charge Waves in Mismatched Beams space-charge, electron, focusing, emittance 3272
 
  • B. R. Poole, D.T. Blackfield, Y.-J. Chen, J.R. Harris
    LLNL, Livermore, California
  • P.G. O'Shea
    UMD, College Park, Maryland
 
 

Funding: This work performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344.


Mismatch oscillations resulting from the propagation of space charge waves in intense beams may lead to halo generation and possible beam loss, and modify longitudinal beam dynamics. These oscillations have amplitudes and frequencies different from that of the main beam and are particularly important in machines such as the University of Maryland Electron Ring (UMER), in which the beam dynamics scale to parameters associated with heavy ion fusion drivers. We use the particle-in-cell (PIC) code, LSP, to simulate space charge wave dynamics in an intense electron beam propagating in a smooth focusing channel with 2-D cylindrical symmetry. We examine the evolution of linear and nonlinear density perturbations in the UMER parameter range for both matched and mismatched beams. Comparisons between LSP simulations and numerical models are presented.

 
TH5PFP037 Spectral-Element Discontinuous Galerkin (SEDG) Simulations with a Moving Window Algorithm for Wakefield Calculations cavity, wakefield, space-charge, electromagnetic-fields 3278
 
  • M. Min, P.F. Fischer
    ANL, Argonne
 
 

We developed a moving window algorithm for the SEDG time-domain code, NekCEM, for wake field calculations. NekCEM is a highly efficient and spectrally accurate electromagnetic solver using the spectral element discontinuous Galerkin (SEDG) method based on body-fitted spectral element hexahedral meshes. When the domain of interest is around a moving bunch within a certain distance, one does not need to carry out full domain simulations. Moving window approach has been a natural consideration in such circumstance to have significant reduction in computational cost for the conventional low-order methods such as FDTD method. However, there have not been studies on the high-order methods, especially the SEDG method, based on the moving window approach. We implemented 3D moving window option for wake field calculations on various conducting cavities including the 9-cell TESLA cavity. We will demonstrate the performance of the SEDG simulations on moving window meshes.

 
TH5PFP039 Solving Vlasov Equation for Beam Dynamics Simulation plasma, space-charge, emittance, proton 3284
 
  • J. Xu, B. Mustapha, J.A. Nolen, P.N. Ostroumov
    ANL, Argonne
 
 

Funding: This work was supported by the U.S. Department of Energy, Office of Nuclear Physics, under Contract No. DE-AC02-06CH11357.


Kinetic space plasma simulations are dominated by PIC (Particle-In-Cell) codes. Due to the inherent noise in PIC simulations, interest in directly solving the Vlasov equation is increasing. With the fast development of supercomputers, this is becoming more realistic. We present our preliminary work on solving the Vlasov equation for beam dynamics simulations*. A high order Spectral Element Method has been applied to achieve high accuracy, easy interpolation, and parallelization. Due to the inherent instability of the Vlasov equation, a spectral filter has been added and mass conservation has been satisfied. The proposed algorithms were validated on 1D1V simulations. A paraxial model of the Vlasov equation (2D2V) has also been studied and compared with PIC simulations at ANL using the BG/P supercomputer.


*J. Xu, P. Ostroumov and J. Nolen, “Highly Scalable Parallel Algorithm for 2D2V Vlasov Equation with High Order Spectral Element Method”, poster on SC08, Austin, Texas, Nov.15-20, 2008.

 
TH5PFP040 Optical Matching of EMMA Cell Parameters Using Field Map Sets lattice, closed-orbit, resonance, acceleration 3287
 
  • Y. Giboudot
    Brunel University, Middlesex
  • F. Méot
    CEA, Gif-sur-Yvette
 
 

The Non Scaling FFAG EMMA lattice allows a important displacement of the magnets in the radial direction. From this peculiarity, interesting studies of beam dynamics can be performed comparing simulated and experimental results. Being able to study a specific resonance, choosing a certain set of parameters for the lattice is really challenging. Simulations have been done integrating particle trajectories with Zgoubi through Magnetic Field Map created with OPERA. From a chosen tune evolution, one can find the corresponding magnets' configuration required by interpolating between a various sets of Field Map. Relative position and strength of the magnets are degrees of freedom. However, summing field maps requires a special care since the real magnetic field created by two magnets is not obviously linearly dependent on each single magnet. For this reason, frequently used hard edge and fringe field models may not be accurate enough. This linearity of the magnetic field has been studied directly through OPERA finite element method solutions and further on with Zgoubi tracking results.

 
TH5PFP041 Particle Tracking Studies Using Dynamical Map Created from Finite Element Solution of the EMMA Cell quadrupole, lattice, closed-orbit, vacuum 3290
 
  • Y. Giboudot, A. Khan
    Brunel University, Middlesex
  • T.R. Edgecock
    STFC/RAL, Chilton, Didcot, Oxon
  • A. Wolski
    The University of Liverpool, Liverpool
 
 

The unconventional size and the possibility of transverse displacement of the magnets in the EMMA non-scaling FFAG motivates a careful study of particle behavior within the EMMA ring. The magnetic field map of the doublet cell is computed using a Finite Element Method solver; particle motion through the field can then be found by numerical integration, using (for example) OPERA, or ZGOUBI. However, by obtaining an analytical description of the magnetic field (by fitting a Fourier-Bessel series to the numerical data) and using a differential algebra code, such as COSY, to integrate the equations of motion, it is possible to produce a dynamical map in Taylor form. This has the advantage that, after once computing the dynamical map, multi-turn tracking is far more efficient than repeatedly performing numerical integrations. Also, the dynamical map is smaller (in terms of computer memory) than the full magnetic field map; this allows different configurations of the lattice, in terms of magnet positions, to be represented very easily using a set of dynamical maps, with interpolation between the coefficients in different maps*.


*yoel.giboudot@stfc.ac.uk

 
TH5PFP042 Simulation Studies on the Electron Cloud Instability in the CSNS Ring electron, proton, vacuum, beam-losses 3293
 
  • N. Wang, Y.D. Liu, Q. Qin
    IHEP Beijing, Beijing
 
 

The electron proton (e-p) instability has been observed in many proton accelerators. It will induce transverse beam size blow up, cause beam loss and restrict the machine performance. A simulation code is developed to study the electron proton instability in the China Spallation Neutron Source (CSNS) ring. The results of numerical simulation of the electron cloud formation and the electron proton instability are presented.

 
TH5PFP043 Density Estimation Techniques for Charged Particle Beams with Applications to Microbunching Instability synchrotron 3296
 
  • G. Bassi
    Cockcroft Institute, Warrington, Cheshire
  • G. Bassi
    The University of Liverpool, Liverpool
  • B. Terzić
    Northern Illinois University, DeKalb, Illinois
 
 

We discuss various density estimation techniques to represent charge particle distributions in beam dynamics simulation codes. A detailed analysis of the different methods shows that for an accurate, reliable and efficient modeling of microbunching instability a careful control of numerical noise is required. In particular, we compare a standard particle-in-cell scheme plus denoising via wavelets thresholding with a meshless Monte-Carlo method used in statistical estimation. We inplement them in a Vlasov-Maxwell solver and show results for FELs systems.

 
TH5PFP046 Condor as a Resource for Accelerator Research klystron, electron, emittance, focusing 3303
 
  • J.D.A. Smith
    Cockcroft Institute, Warrington, Cheshire
  • J. Kewley
    STFC/DL, Daresbury, Warrington, Cheshire
  • C. Lingwood
    Cockcroft Institute, Lancaster University, Lancaster
  • J.W. McKenzie
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

This work reports on the developments of a computational infrastructure framework that aids achievement of computational research objectives. Examples from a broad range of accelerator problems will be presented, along with ways in which the workflow can be modified.

 
TH5PFP047 Electron Cloud Modeling Considerations at CesrTA electron, space-charge, photon, positron 3306
 
  • J.R. Calvey, J.A. Crittenden, G. Dugan, M.A. Palmer
    CLASSE, Ithaca, New York
  • C.M. Celata
    LBNL, Berkeley, California
 
 

Funding: Support provided by the US National Science Foundation and the US Department of Energy


The Cornell Electron Storage Ring (CESR) has recently begun operation as a test accelerator for next generation linear collider damping rings. This program, known as CesrTA, includes a thorough investigation of synchrotron radiation generated electron cloud effects. CESR is capable of operating with a variety of bunch patterns and beam currents, as well as with both electron and positron beams. Understanding the buildup of the cloud under these conditions requires the use of well validated simulation programs. This paper will discuss three such programs- POSINST, ECLOUD and CLOUDLAND, which have been benchmarked against each other in parameter regimes relevant to CesrTA operating conditions, with the aim of understanding systematic differences in the calculations.

 
TH5PFP048 Collimating Touschek Particles in an Energy Recovery Linear Accelerator scattering, lattice, linac, shielding 3309
 
  • M. P. Ehrlichman, G.H. Hoffstaetter
    CLASSE, Ithaca, New York
 
 

Funding: This work was supported by the National Science Foundation.


The theories of beam loss and emittance growth by Touschek and intra-beam scattering formulated for beams in storage rings have recently been extended to linacs. In most linacs, these effects are not relevant, but they become important in Energy Recovery Linacs (ERLs) not only because of their large current, but also because the deceleration of the spent beam increases the relative energy deviation and transverse oscillation amplitude of the scattered particles. In this paper, we describe a methodology for designing a collimator scheme to control where scattered particles are lost. The methodology is based on Touschek particle generation and tracking simulations implemented in {\tt BMAD}, Cornell's beam dynamics code. The simulations give the locations where scattering occurs and the locations where the scattered particles are lost. The simulations are used to determine the trajectory of the scattered particles, which are analyzed to determine optimal locations for collimators.

 
TH5PFP050 Fast Multipole Approximation of 3D Self Fields Effect in High Brightness Electron Beams multipole, target, space-charge, electron 3315
 
  • M. Quattromini, M. Del Franco, L. Giannessi
    ENEA C.R. Frascati, Frascati (Roma)
 
 

In this paper the Fast Multipole Approximation is described with regard to the problem of modelling self fields effects in low emittance, high brightness electron beams of interest for future accelerators and light sources. This well established technique is known to scale as O(N) or O(N log N) (depending on details of the implementation) with the number of particles involved in the simulation. Performances and results as a standalone technique or as a method for for fast calculation of boundary conditions together with other approaches based on PDEs are discussed, along with details of a parallel implementation in the tracking code Tredi.

 
TH5PFP051 Numerical Algorithms for Dispersive, Active, and Nonlinear Media with Applications to the PASER resonance, acceleration, wakefield, laser 3318
 
  • P. Schoessow, A. Kanareykin
    Euclid TechLabs, LLC, Solon, Ohio
  • L. Schächter
    Technion, Haifa
 
 

Funding: Work supported by the US Department of Energy.


The PASER is one of the first advanced accelerator modeling applications that requires a more sophisticated treatment of dielectric and paramagnetic media properties than simply assuming a constant permittivity or permeability. So far the PASER medium has been described by a linear, frequency-dependent, single-frequency, scalar dielectric function. We have been developing algorithms to model the high frequency response of dispersive, active, and nonlinear media with an emphasis on areas most useful for PASER simulations. The work described also has applications for modeling of other electromagnetic problems involving realistic dielectric and magnetic media. Results to be reported include treatment of multiple Lorentz resonances based on auxiliary differential equation, Fourier, and hybrid approaches, and Kerr, Brillouin, and Raman optical nonlinearities.

 
TH5PFP052 Electron Cloud Simulations for ANKA electron, vacuum, undulator, dipole 3321
 
  • U. Iriso
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
  • S. Casalbuoni
    FZK, Karlsruhe
  • G. Rumolo, F. Zimmermann
    CERN, Geneva
 
 

One of the key issues for the developments of superconducting insertion devices is the understanding of the beam heat load in the vacuum chamber. The beam heat load observed in the superconducting cold bore undulator installed in the ANKA storage ring is higher than the one predicted by the synchrotron radiation and resistive wall heating. A non linear increase of the dynamic pressure with the beam current is also observed in the cold bore. In order to investigate whether the nature of these effects is due to an electron cloud formation, we have performed several simulations using the ECLOUD code.

 
TH5PFP053 Graphical Front-End and Object-Oriented Design for IonEx, an Ion Extraction Modeling Code ion, extraction, emittance, electron 3324
 
  • L. Grubert, N. Barov, B. Cluggish, S. Galkin, J.S. Kim
    Far-Tech, Inc., San Diego, California
 
 

Funding: DOE


IonEx is a new hybrid, meshless, cross-platform, 2D code which can model the extraction of ions from a plasma device. The application includes a user-friendly Graphical User Interface (GUI), which contains a geometry editor for specifying the domain. The design of IonEx utilizes the object-oriented functionality of C++, which provides an efficient means of incorporating a magnetic field, an arbitrary geometry, and an unlimited number of ion species into a simulation. Visualization of the resulting trajectories and emittances is accomplished through the GUI; openGL is used to accelerate the graphics. In this paper we will briefly review the physics and computational methods used, highlight important aspects of the object-oriented design, discuss the primary features of the GUI, describe the current status of IonEx, and present some simulation results.

 
TH5PFP054 Validation and Application of GEM (General ECRIS Modeling) ion, ECR, plasma, ECRIS 3327
 
  • L. Zhao, B. Cluggish, J.S. Kim
    Far-Tech, Inc., San Diego, California
  • R.C. Pardo, R.C. Vondrasek
    ANL, Argonne
 
 

Funding: This work is supported by the US DOE SBIR program


GEM, developed by FAR-TECH Inc, is a self consistent hybrid code to simulate general ECRIS plasma. It calculates EDF (electron distribution function) using a bounce-averaged Fokker-Planck code and calculates the ion flow using a fluid code, which has been modified to implement new boundary settings including fixed boundary ion velocities or fixed sheath potentials at both ends of the device. Extensive studies on the convergence and performance of the code have been performed. Also, GEM has been connected to MCBC (Monte Carlo beam capture) code and the validations of the code using ANL ECR-I charge breeding data and other published experiments are underway. The typical converged solutions of GEM and the comparisons with the experiments will be presented and discussed.

 
TH5PFP056 Using PARMILA 2 with the Particle Beam Optics Laboratory DTL, optics, linac, proton 3333
 
  • G.H. Gillespie, W. Hill
    G.H. Gillespie Associates, Inc., Del Mar, California
 
 

A PARMILA 2 Module has been developed for the Particle Beam Optics Laboratory (PBO Lab). PARMILA 2 is a FORTRAN program used to both design and simulate radiofrequency ion linear accelerators. The program can be used to design radiofrequency accelerators that include drift tube linac (DTL) structures, coupled cavity linac (CCL) structures, coupled-cavity drift tube linac (CC-DTL) structures, and superconducting accelerator structures. PARMILA 2 can also be used to simulate beams in these structures and in transport lines that with magnetic, radiofrequency and electrostatic beam optics elements. PBO Lab provides a sophisticated graphic user interface (GUI) for multiple optics codes. From the same familiar interface users can run TRANSPORT, TURTLE, MARYLIE, TRACE 3-D and DECAY-TURTLE. PARMILA 2 now joins this suite of optics codes available as PBO Lab Modules. New PBO Lab tools have been developed to assist users in utilizing different optics codes to simulate and validate the performance of an accelerator designed with PARMILA 2. An overview of the new PARMILA 2 module and associated new tools is presented and some of the GUI features are illustrated.

 
TH5PFP058 RFQ Particle Dynamic Simulation Development rfq, multipole, acceleration 3339
 
  • J.M. Maus, U. Bartz, R.A. Jameson, N. Mueller, A. Schempp
    IAP, Frankfurt am Main
 
 

For the development of high energy and high duty cycle RFQs accurate particle dynamic simulation tools are important optimize designs especially in high current applications. To describe the external fields in RFQs the Poisson equation has to be solved taking the boundary conditions into account. In the newly developed subroutines this is done by using a finite difference method on a grid. The results of this improvement are shown and compared to the old two term and multipol expansions.

 
TH5PFP062 Numerical Study of Collective Effects for Muon Beams space-charge, emittance, collective-effects, target 3345
 
  • D. Huang
    IIT, Chicago, Illinois
  • D.M. Kaplan
    Illinois Institute of Technology, Chicago, Illinois
  • K.Y. Ng
    Fermilab, Batavia
  • T.J. Roberts
    Muons, Inc, Batavia
 
 

Funding: Supported in part by USDOE Contract DE-FG02-6ER86281


The study of Muon beam optics is crucial for future Neutrino Factory and Muon Collider facilities. At present, the GEANT4-based simulation tools for Muon beam tracking such as G4beamline and G4MICE are based on single particle tracking without collective effects taken into account. However, it is known that collective effects such as space charge and wakefields for muons (in matters or vacuum) are not ignorable. As the first step, space charge computation has been implemented into muon tracking. The basic algorithm is particle to particle interactions through retarded electro-magnetic fields. The momentum impulse by collective effects is imposed on every particle at each collective step, and the G4beamline main code is used for tracking. Comparisons to LANL Parmela are illustrated and analyzed. Optimizations of the algorithm are also underway to gain less computing time and more accuracy. Moreover, the idea of enhancing ionization cooling efficiency by utilizing the collective effect due to polarized charges in matter appears to be possible, and the preliminary estimation has been done.

 
TH5PFP064 Time-Retardation Effect Causing Beamloss in the RF Photoinjector space-charge, beam-losses, laser, cathode 3351
 
  • C.S. Park, M. Hess
    IUCF, Bloomington, Indiana
  • W. Gai, J.G. Power
    ANL, Argonne
 
 

Funding: Supported in part by DOE(DE-FG029ER40747) and in part by NSF(PHY-0552389)


Near the cathode in a photoinjector, the electron beam is emitted with low energy, and its dynamics are strongly affected by the beam's space-charge fields. This can cause beam loss at the cathode due to virtual cathode formation. In general, a fully electromagnetic code can correctly predict the beam space-charge fields, beam dynamics, and beam loss. However, an electrostatic type algorithm would overestimate the space-charge fields since it does not incorporate relativistic time-retardation effects which limit the size of the fields near the cathode. IRPSS (Indiana RF Photocathode Source Simulator) can calculate the electromagnetic space-charge fields using a Green’s function method to a high-precision, and can track beam dynamics in the RF photoinjector. Using IRPSS, we simulated the beam dynamics and beam loss near the cathode for the Argonne Wakefield Accelerator 1.3 GHz gun* and compared those results to electrostatic codes, such as PARMELA and ASTRA.


*P. Schoessow, PAC 2009.

 
TH5PFP067 Longitudinal Phase Space Tomography at J-PARC RCS synchrotron, injection, proton, acceleration 3358
 
  • M. Yoshimoto, N. Hayashi, M. Kawase, F. Tamura, M. Yamamoto
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  • M. Yoshii
    KEK/JAEA, Ibaraki-Ken
 
 

In order to observe two-dimensional beam profiles in the longitudinal phase space, the reconstruction techniques with the computer tomography algorithms can be adopted at the J-PARC RCS. On the assumption that the longitudinal profiles should not be disturbed for one period of the synchrotron oscillation, such two-dimensional profiles can be reconstructed easily from one-dimensional bunch beam profiles, which are measured for every turn by the wall current monitor. In this presentation, we introduce the experimental results and the comparison to the longitudinal beam tracking simulation, and we discuss the technical issues and applicability of this longitudinal tomography techniques.

 
TH5PFP068 Simulation of the Alignment of Linear Accelerators laser, emittance, alignment, linac 3361
 
  • J. Dale, A. Reichold
    JAI, Oxford
 
 

The alignment of the next generation of linear accelerators will be much more critical than that of currently existing machines. This is especially true for very long machines with ultra low emittance beams; such as the ILC and CLIC. The design and study of such machines will require a large number of simulations. However; full simulation of misalignment currently requires computer programs which are very resource intensive. A model which can be used to rapidly generate reference networks with the required statistical properties will be presented. The results for emittance growth in the ILC main linac using the model with Dispersion Matched Steering (DMS) applied are also shown.

 
TH5PFP070 Application of the Adaptive Mesh Refinement Technique to Particle-in-Cell Simulations of Beams and Plasmas plasma, laser, wakefield, electron 3364
 
  • J.-L. Vay, C.G.R. Geddes
    LBNL, Berkeley, California
  • A. Friedman, D.P. Grote
    LLNL, Livermore, California
 
 

Funding: Supported by the US-DOE under Contracts DE-AC02-05CH11231 and DE-AC52-07NA27344, and a DOD SBIR Phase II. Used resources of NERSC, supported by the US-DOE under Contract DE-AC02-05CH11231.


The development of advanced accelerators often involves the modeling of systems that involve a wide range of scales in space and/or time, which can render such modeling extremely challenging. The Adaptive Mesh Refinement technique can be used to significantly reduce the requirements for computer memory and the number of operations. Its application to the fully self-consistent modeling of beams and plasmas is especially challenging, due to properties of the Vlasov-Maxwell system of equations. Most recently, we have begun to explore the application of AMR to the modeling of laser plasma wakefield accelerators (LWFA). For the simulation of a 10GeV LWFA stage, the wake wavelength is O[100μm] while the electron bunch and laser wavelength are typically submicron in size. As a result, the resolution required for different parts of the problem may vary by more than two orders of magnitude in each direction, corresponding to up to 6 orders of magnitude of possible (theoretical) savings by use of mesh refinement. We present a summary of the main issues and their mitigations, as well as examples of application in the context of LWFA and similar beam-plasma interaction setup.

 
TH5PFP072 Simulating an Acceleration Schedule for NDCX-II acceleration, solenoid, lattice, ion 3368
 
  • W. M. Sharp, A. Friedman, D.P. Grote
    LLNL, Livermore, California
  • E. Henestroza, M. Leitner, W.L. Waldron
    LBNL, Berkeley, California
 
 

Funding: Work performed under the auspices of US Department of Energy by LLNL under Contract DE- AC52-07NA27344 and by LBNL under Contract DE-AC03-76SF00098.


The Virtual National Laboratory for Heavy-Ion Fusion is developing a physics design for NDCX-II, an experiment to study warm dense matter heated by ions near the Bragg-peak energy. Present plans call for using about thirty induction cells to accelerate 30 nC of Li+ ions to more than 3 MeV, followed by neutralized drift-compression. To heat targets to useful temperatures, the beam must be compressed to a sub-millimeter radius and a duration of about 1 ns. An interactive 1-D particle-in-cell simulation with an electrostatic field solver, acceleation-gap fringe fields, and a library of realizable analytic waveforms has been used for developing NDCX-II acceleration schedules. Multidimensional source-to-final-focus simulations with the particle-in-cell code Warp have validated this 1-D model and have been used both to design transverse focusing and to compensate for injection non-uniformities and 3-D effects. Results from this work are presented, and ongoing work to replace the analytic waveforms with output from circuit models is discussed.

 
TH5PFP073 Ion Effect Issues in PETRA III ion, feedback, damping, electron 3371
 
  • G.X. Xia
    MPI-P, München
  • M. Ivanyan
    CANDLE, Yerevan
  • K. Manukyan, K.A. Sargsyan
    YSU, Yerevan
  • R. Wanzenberg
    DESY, Hamburg
 
 

At DESY the PETRA accelerator has been converted into a new 3rd generation high-brilliance synchrotron radiation facility called PETRA III. For the first commissioning in spring 2009 a positron beam is used. In the future it is also foreseen to operate the synchrotron light source with an electron beam. Ion effects pose a potential problem to the electron beam operation of PETRA III. In this paper, a weak-strong simulation code is employed to study the ion effect issues in detail for different operation scenarios.

 
TH5PFP074 Putting Space Charge into G4beamline space-charge, solenoid, emittance, electron 3374
 
  • K.B. Beard, T.J. Roberts
    Muons, Inc, Batavia
 
 

Funding: Supported in part by USDOE Contract DE-FG02-6ER86281.


The G4beamline program is based on the well-established Geant4 toolkit used to simulate the interactions of particles and photons with matter. Until now, only a single particle at a time could be tracked and there are no interactions between particles. Recent designs for high pressure RF cavities and other novel devices achieving extreme muon cooling require that the effect of space charge be included in the simulations. A new tracking manager in G4beamline propagates a number of particles (typically 1,000-10,000) in parallel, stepping all particles in time. This allows all of the usual Geant4 physics interactions to be applied, plus collective computations. A simple macroparticle-based model is used to represent ~108 charges with an ellipsoidal charge density. At intervals the appropriate macroparticle size and shape are recalculated, the electric and magnetic fields are determined, and an impulse is applied to the simulated particles. Comparisons to standard space charge codes are presented.

 
TH5PFP075 Simulation Tools for the Muon Collider Design Feasibility Study collider, emittance, proton, controls 3377
 
  • T.J. Roberts
    Muons, Inc, Batavia
  • R.C. Fernow
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported in part by USDOE STTR Grant DE-FG02-08ER86281 and DE AC02 98CH10886.


The U.S. muon collider community is mobilizing itself to produce a “Design Feasibility Study” (DFS) for a muon collider. This is happening on an aggressive schedule and must include the best possible simulations to support and validate the technical design. The DFS for a muon collider will require innovative new approaches to many aspects of accelerator design, and the simulations to support it will require tools with features and capabilities that are equally innovative and new. Two computer programs have emerged as the preferred and most commonly used simulation tools within the muon collider community: ICOOL (primary author: Dr. Fernow), and G4beamline (primary author: Dr. Roberts). We describe the ongoing development and testing of both tools for the DFS, including a common suite of tests to ensure that both tools give accurate and realistic results, as well as innovative user-friendly interfaces with emphasis on graphical user interfaces and windows.

 
TH5PFP076 Particle Tracking in Matter Dominated Beam Lines collider, target, space-charge, factory 3380
 
  • T.J. Roberts, K.B. Beard
    Muons, Inc, Batavia
  • S. Ahmed, D.M. Kaplan, L.K. Spentzouris
    Illinois Institute of Technology, Chicago, Illinois
  • D. Huang
    IIT, Chicago, Illinois
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-06ER86281


Most computer programs that calculate the trajectories of particles in accelerators assume that the particles travel in an evacuated chamber. The development of muon beams, which are needed for muon colliders and neutrino factories and are usually required to pass through matter, is limited by the lack of user-friendly numerical simulation codes that accurately calculate scattering and energy loss in matter. Geant4 is an internationally supported tracking toolkit that was developed to simulate particle interactions in large detectors for high energy physics experiments, and includes most of what is known about the interactions of particles and matter. Geant4 has been partially adapted in a program called G4beamline to develop muon beam line designs. The program is now being developed and debugged by a larger number of accelerator physicists studying muon cooling channel designs and other applications. Space-charge effects and muon polarization are new features that are being implemented.

 
TH5PFP078 Low-Frequency Time Domain Numerical Studies of Transition Radiation in a Cylindrical Waveguide radiation, electromagnetic-fields, diagnostics, linac 3383
 
  • X. Sun, G. Decker
    ANL, Argonne
 
 

Transition radiation is frequently used to determine the time profile of a bunched relativistic particle beam. Emphasis is usually given to diagnostics sensitive to wavelengths in the infrared-to-optical portion of the spectrum. In this study, CST Particle Studio simulations are used to make quantitative statements regarding the low-frequency (DC to microwave) behavior of coherent transition radiation from a mirror inclined at 45 degrees relative to the particle beam trajectory. A moving Gaussian bunch confined within a cylindrical beam pipe is modeled. Simulation results are presented.

 
TH5PFP080 Results from a Test Fixture for Button BPM Trapped Mode Measurements impedance, resonance, coupling, pick-up 3389
 
  • P. Cameron, B. Bacha, A. Blednykh, I. Pinayev, O. Singh
    BNL, Upton, Long Island, New York
 
 

Three-dimensional electromagnetic simulations have suggested a variety of measures to mitigate the problem of button BPM trapped mode heating. A test fixture, using a combination of commercial-off-the-shelf and custom machined components, was assembled to validate the simulations. We present details of the fixture design, measurement results, and a comparison of the results with the simulations.

 
TH5PFP083 Eddy Current Shielding by Electrically Thick Vacuum Chambers vacuum, feedback, multipole, power-supply 3398
 
  • B. Podobedov, L. Ecker, D.A. Harder, G. Rakowsky
    BNL, Upton, Long Island, New York
 
 

We investigate AC response of accelerator vacuum chambers to external magnetic field, when the wall thickness is comparable or greater than the skin depth. Good agreement was established between experimental measurements, analytical modeling, and ANSYS simulations. Based on the results we suggest a transfer function model for electrically thick vacuum chambers with arbitrary transverse cross-section.

 
TH5PFP084 Computation of Resistive Wakefields for Collimators wakefield, emittance, higher-order-mode, impedance 3401
 
  • R.J. Barlow, A.M. Toader
    UMAN, Manchester
 
 

A technique has been developed which enables the calculation of resistive particle wake effects. The technique can simply be calculated to any order, and is easy and quick to evaluate. No assumptions are made about the range of the interaction, but this is especially useful for short range effects. We show how the exact evaluation compares with various common approximations for some simple cases, and implement the technique in the Merlin and PLACET simulation programs. The extension from cylindrical to rectangular apertures is highlighted.

 
TH5PFP086 About Non Resonant Perturbation Field Measurement in Standing Wave Cavities cavity, resonance, brilliance, RF-structure 3407
 
  • A. Mostacci, R. Da Re, L. Palumbo
    Rome University La Sapienza, Roma
  • D. Alesini, L. Ficcadenti, B. Spataro
    INFN/LNF, Frascati (Roma)
 
 

We discuss the use of non resonant bead pull technique for measuring fields in standing wave accelerating structures. From the Steele perturbation theory, one can derive the relation between the magnitude and phase of the field in the cavity and the complex reflection coefficient. The effect of the bead size, the calibration of the bead and the comparison with the more common resonant techniques are addressed. As an example, we discuss the measurement on a X-band bi-periodic cavity proposed for linearizing emittance at the Frascati photo-injector SPARC.

 
TH5PFP089 Trapped Mode Study for a Rotatable Collimator Design for the LHC Upgrade vacuum, HOM, damping, collimation 3416
 
  • L. Xiao, C.-K. Ng, J.C. Smith
    SLAC, Menlo Park, California
  • F. Caspers
    CERN, Geneva
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


A rotatable collimator is proposed for the LHC phase II collimation upgrade. When the beam crosses the collimator, trapped modes will be excited that result in beam energy loss and collimator power dissipation. Some of the trapped modes can also generate transverse kick on the beam and affect the beam operation. In this paper the parallel eigensolver code Omega3P is used to search for all the trapped modes below 2GHz in the collimator, including longitudinal modes and transverse modes. The loss factors and kick factors of the trapped modes are calculated as function of the jaw positions. The amplitude ratio between transverse and longitudinal trapped mode intensity can be used as a direct measure of the position of the beam. We present simulation results and discuss the results.

 
TH5PFP091 Comparison of Analytical and Numerical Results for Broadband Coupling Impedance impedance, coupling, wakefield, vacuum 3420
 
  • L. Haenichen, W.F.O. Müller, T. Weiland
    TEMF, TU Darmstadt, Darmstadt
  • A.M. Al-Khateeb, O. Boine-Frankenheim
    GSI, Darmstadt
 
 

Funding: This work is supported by the GSI.


Beam coupling impedances have been identified as an appropriate quantity to describe collective instabilities caused through beam-induced fields in heavy ion synchrotron accelerators such as the SIS-18 at the planned SIS-100 at the GSI facility. The impedance contributions caused by the multiple types of beamline components need to be determined to serve as input condition for later stability studies. This paper will present an approach exploiting the abilities of commercial FDTD wake codes such as CST PARTICLE STUDIO® for a benchmark problem with cylindrical geometry. Since exact analytical formulae are available, the obtained numerical results will be compared. Special attention is paid towards the representation of the particle beam as the source of the EM fields and conductive losses.

 
TH5PFP093 Benchmark of Different Electromagnetic Codes for the High Frequency Calculation cavity, vacuum, superconducting-RF, electromagnetic-fields 3426
 
  • K. Tian, G. Cheng, F. Marhauser, H. Wang
    JLAB, Newport News, Virginia
  • C.D. Zhou
    Tech-X, Boulder, Colorado
 
 

Funding: Authored by Jefferson Science Associates, LLC under U.S. DOE Contract No. DE-AC05-06OR23177.


In this paper, we present benchmarking results for high-class 3D electromagnetic (EM) codes in designing RF cavities today. These codes include Omega3P [1], VORPAL [2], CST Microwave Studio [3], Ansoft HFSS [4], and ANSYS [5]. Two spherical cavities are selected as the benchmark models. We have compared not only the accuracy of resonant frequencies, but also that of surface EM fields, which are critical for superconducting RF cavities. By removing degenerated modes, we calculate all the resonant modes up to 10 GHz with similar mesh densities, so that the geometry approximation and field interpolation error related to the wavelength can be observed.

 
TH5RFP001 Development of Metamaterials for Cherenkov Radiation Based Particle Detectors wakefield, radiation, proton, resonance 3432
 
  • S.P. Antipov, W. Gai, J.G. Power
    ANL, Argonne
  • A. Kanareykin, P. Schoessow
    Euclid TechLabs, LLC, Solon, Ohio
  • G. Semouchkin, E. Semouchkina
    PSU, University Park, Pennsylvania
  • A.V. Tyukhtin
    Saint-Petersburg State University, Saint-Petersburg
 
 

Funding: DOE


Metamaterials (MTMs) are periodic artificially constructed electromagnetic structures. The periodicity of the MTM is much smaller than the wavelength of the radiation being transported. With this condition satisfied, MTMs can be assigned an effective permittivity and permeability. Areas of possible application of MTMs in accelerator science are Cherenkov detectors and wakefield devices. MTMs can be designed to be anisotropic and dispersive. The combination of engineered anisotropy and dispersion can produce a Cherenkov radiation spectrum with a different dependence on particle energy than conventional materials. This can be a basis for novel non-invasive beam energy measurements. We report on progress in the development of these media for a proof-of-principle demonstration of a metamaterial-based beam diagnostic.

 
TH5RFP002 Simulations of the Beam Loss Monitor System for the LCLS Undulator Beamline electron, undulator, beam-losses, neutron 3435
 
  • J.C. Dooling, W. Berg, A.F. Pietryla, B.X. Yang
    ANL, Argonne
  • H.-D. Nuhn
    SLAC, Menlo Park, California
 
 

Funding: Work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under contract number DE-AC02-06CH11357.


Simulations of the beam loss monitor (BLM) system built at the Advanced Photon Source (APS) for the Linear Coherent Light Source (LCLS) have been carried out using the Monte Carlo particle tracking code MARS. Cerenkov radiation generated by fast electrons in the quartz radiator of the BLM produces the signal used to estimate beam loss and dose in the LCLS undulator magnets. The calibration of the BLM signal with radiation components that cause undulator damage is the goal of the simulation effort. Beam loss has been simulated for several scenarios including undulator magnets in the normal operating position, “rolled-out” 80 mm from the beamline, and absent altogether. Beam loss is generated when an electron bunch strikes one of two targets: Al foil or carbon wire. In the former case, the foil is placed at OTR33, 85.8 m upstream of the FEL; in the latter, the first undulator beam finder wire (BFW01) position is used just upstream of the first magnet. The LCLS MARS model includes quadrupole focusing between OTR33 and the end of the FEL. The FODO lattice leads to complex loss patterns in the undulators consistent with betatron envelope maximums in both transverse planes.

 
TH5RFP005 Pepper-Pot Based Diagnostics for the Measurement of the 4D Transverse Phase Space Distribution from an RF Photoinjector at the AWA emittance, electron, solenoid, cathode 3444
 
  • J.G. Power, M.E. Conde, W. Gai, W. Liu
    ANL, Argonne
  • P. Piot
    Northern Illinois University, DeKalb, Illinois
 
 

Funding: The work is supported by the U.S. Department of Energy under Contract No. DE-AC02-06CH11357 with Argonne National Laboratory.


Phase space measurements of RF photoinjectors have usually been done with multislit masks or scanning slits. These systems implicitly ignore the correlations between the X and Y planes and thus yield measurements of the projected 2D phase space distributions. In contrast, a grid-patterned pepper-pot is capable of measuring the full 4D transverse phase space distribution, f(x,x',y,y'). 4D measurements allow precise tuning of electron beams with large canonical angular momentum, important for electron cooling and flat beam transformation, as well as zeroing the magnetic field on the photocathode is zero for ultra low emittance applications (e.g. SASE FEL, ERL FEL). In this talk, we report on a parametric set of measurements to characterize the 4D transverse phase space of the 1 nC electron beam from the Argonne Wakefield Accelerator (AWA) RF photoinjector. The diagnostic is simulated with TStep, including the passage of the electron beam trough the mask and tracking of the beamlets to the imaging screen. The phase space retrieval algorithm is then bench marked against simulations and measurements.

 
TH5RFP008 Upgrade of the Beam Position Monitors at the Brazilian Synchrotron Light Source vacuum, storage-ring, synchrotron, injection 3453
 
  • S.R. Marques, O.R. Bagnato, R.H.A. Farias, F. R. Francisco, R.T. Neuenschwander, F. Rodrigues, A.L. Rosa, R.M. Seraphim, P.F. Tavares, M.M. Xavier
    LNLS, Campinas
 
 

We describe the development of a new button-type beam position monitor (BPM) for the Brazilian Synchrotron Light Source (LNLS) electron storage ring. One third of the storage ring stripline BPMs were replaced whit this new model, which counts on bellows, temperature stabilization and new support stands in order achieve improved mechanical stability. Finally, in-vacuum heat absorbers were installed at the upstream vacuum tubes of the bending magnets to minimize the vacuum chamber motion due to the high thermal load. We also present performance results.

 
TH5RFP011 BPM Button Optimization to Minimize Distortion due to Trapped Mode Heating impedance, pick-up, synchrotron, resonance 3462
 
  • P. Cameron, A. Blednykh, B.N. Kosciuk, I. Pinayev, V. Ravindranath, O. Singh
    BNL, Upton, Long Island, New York
 
 

The thermal distortion resulting from BPM button trapped mode heating is potentially problematic for achieving the high precision beam position measurement needed to provide the sub-micron beam position stability required by light source users. We present a button design that has been thermo-mechanically optimized via material selection and component geometry to minimize this thermal distortion. Detailed electromagnetic analysis of the button geometry is presented elsewhere in these proceedings.

 
TH5RFP018 Effects of High Proton Fluences on CZT Detectors radiation, proton, photon, linac 3482
 
  • N. Simos, A. Aronson, A.E. Bolotnikov, G.S. Camarda, C. Copeland, R. James, H. Ludewig
    BNL, Upton, Long Island, New York
 
 

The effects of high fluences of energetic charged particles on CdZnTe detectors have been studied and are reported in this paper. Specifically, 200 MeV protons of the Brookhaven National Laboratory LINAC were used to bombard a set of CdZnTe detector crystals to fluences as high as 2.6x1016 protons/cm2. Following exposure a set of past-irradiation analyses were conducted to quantify the effects. These include (a) gamma-ray spectra analysis using a high-purity germanium detector in an effort to assess both the peak position shifting as a function of fluence and the spectral content, (a) resistivity and leakage current measurements, and (c) manifestation of radiation damage in the crystal microstructure. In addition, and based on the irradiation parameters used, a numerical prediction model was formulated aiming to benchmark the observed isotopes.

 
TH5RFP031 Expected Performance of TOTEM BLMs at the LHC proton, hadron, neutron, luminosity 3513
 
  • R. Appleby, R.J. Hall-Wilton, D. Macina, V. Talanov
    CERN, Geneva
 
 

The TOTEM experiment at the LHC will operate at down to 10 σ from the beam in the forward region of the CMS experiment. The associated beam loss monitors (BLMs) are crucial to monitor the position of the detectors and to provide a rapid identification of abnormal beam conditions for machine protection purposes. In this paper, the response of the TOTEM BLMs is considered and the protection thresholds are defined, with calculations made of the expected signal from protons grazing the TOTEM pot as a function of pot distance from the beam, and of the BLM signal from proton collisions at the CMS beam interaction point.

 
TH5RFP032 FLUKA Simulations and SPS Measurements for the LHC BRAN luminosity, proton, neutron, photon 3516
 
  • S.M. White, E. Bravin
    CERN, Geneva
 
 

The LHC collision rate monitors (BRAN) will be used to monitor and optimize the luminosity at the four interaction points (IP). Depending on the expected level of luminosity for a given IP two different designs have been developed for LHC. At IP1 and IP5, the high luminosity experiments, the BRAN consist of fast ionization chambers and at IP2 and IP8, where the collision rate will be smaller, they consist of fast polycristalline-CdTe detectors. A better understanding of the performances of those detectors can be provided by detailed tracking simulations of the collision products coming from the IP within the detector. Here we report about the results of simulations done with FLUKA as well as a comparison with measurements done in the SPS.

 
TH5RFP033 Ringing in the Pulse Response of Long and Wideband Coaxial Transmission Lines due to Group Delay Dispersion impedance, linac, vacuum, shielding 3519
 
  • G. Kotzian, F. Caspers, S. Federmann, W. Höfle
    CERN, Geneva
  • R. De Maria
    BNL, Upton, Long Island, New York
  • G. Kotzian
    Graz University of Technology (TUG), Signal Processing and Speech Communication Laboratory (SPSC), Graz
 
 

In particle accelerators coaxial cables are commonly used to transmit wideband beam signals covering many decades of frequencies over long distances. Those transmission lines often have a corrugated outer and/or inner conductor. This particular construction exhibits a significant amount of frequency dependent group delay variation. A comparison of simulations based on theoretical models and S11 and S21 network analyzer measurements up to 2.5 GHz is presented. It is shown how the non-linear phase response and varying group delay leads to ringing in the pulse response and subsequent distortion of signals transmitted through such coaxial transmission lines.

 
TH5RFP035 Energy Deposition Simulations and Measurements in an LHC Collimator and Beam Loss Monitors proton, beam-losses, injection, collimation 3525
 
  • T.T. Boehlen, R.W. Assmann, C. Bracco, B. Dehning, S. Redaelli, Th. Weiler, C. Zamantzas
    CERN, Geneva
 
 

The LHC collimators are protected against beam caused damages by measuring the secondary particle showers with beam loss monitors. Downstream of every collimator an ionisation chamber and a secondary emission monitor are installed to determine the energy deposition in the collimator. The relation between the energy deposition in the beam loss monitor and the collimator jaw is based on secondary shower simulations. To verify the FLUKA simulations the prototype LHC collimator installed in the SPS was equipped with beam loss monitors. The results of the measurements of the direct impact of the 26 GeV proton beam injected in the SPS onto the collimator are compared with the predictions of the FLUKA simulations. In addition simulation results from parameter scans and for mean and peak energy deposition with its dependencies are shown.

 
TH5RFP041 An Improved Retarding Field Analyzer for Electron Cloud Studies electron, vacuum, proton, quadrupole 3540
 
  • C.-Y. Tan, K.L. Duel, R.M. Zwaska
    Fermilab, Batavia
 
 

Funding: Operated by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the United States Department of Energy.


We have designed a retarding field analyzer (RFA) and a rad-hard amplifier which improves the sensitivity over the present RFA installed in the Main Injector. From computer simulations and bench measurements, our RFA will have a 20% improvement in sensitivity compared to the Argonne National Laboratory (ANL) design. And when we couple our RFA to the matched rad-hard amplifier, S/N is also improved.

 
TH5RFP048 Performance of Coded Aperture X-Ray Optics with Low Emittance Beam at CesrTA emittance, optics, photon, vacuum 3561
 
  • J.W. Flanagan, H. Fukuma, S. Hiramatsu, H. Ikeda, K. Kanazawa, T.M. Mitsuhashi, J. Urakawa
    KEK, Ibaraki
  • J.P. Alexander, W.H. Hopkins, B. Kreis, M.A. Palmer, D.P. Peterson
    CLASSE, Ithaca, New York
  • G.S. Varner
    UH, Honolulu, HI
 
 

Funding: Work supported in part by the US-Japan Cooperation Program


We are working on the development of a high-speed x-ray beam profile monitor for high-resolution and fast response for beam profile measurements to be used at CesrTA and SuperKEKB*. The optics for the monitor are based on a technique borrowed from x-ray astronomy, coded-aperture imaging, which should permit broad-spectrum, low-distortion measurements to maximize the observable photon flux per bunch. Coupled with a high-speed digitizer system, the goal is to make turn-by-turn, bunch-by-bunch beam profile measurements. Following initial tests with a low-resolution mask at large beam sizes (vertical size ~200 um), a high-resolution mask has been made for use with low-emittance beams (vertical size ~10 um) at CesrTA. The first performance results of the high-resolution mask on the low-emittance CesrTA beam are presented.


*J.W. Flanagan et al., Proc. EPAC08, Genoa, {10}29 (2008).

 
TH5RFP053 Design and Simulation of the Wire Scanner for Halo Formation Measurements in an Intense Beam RFQ Linac proton, rfq, electron, beam-losses 3573
 
  • Y.F. Ruan
    Institute of High Energy Physics, CAS, Bejing
  • S. Fu, L.X. Han, J. Peng, J.L. Sun, S. Xiao, T.G. Xu, H.S. Zhang, Y.F. Zhang
    IHEP Beijing, Beijing
 
 

A high current proton RFQ accelerator has been constructed in China for the basic study of Accelerator Driven Subcritical System. A new beam line will be set up for the 3.54MeV, 50mA proton beam from the RFQ in order to study beam halo phenomenon. Therefore, 18 wire scanners consist of a thin carbon wire and two scrapers will be installed on the beam line to traverse the entire beam cross-section. So we can experimentally study the beam loss and beam halo. Some simulations results of the heat on the devices by using finite element method software–ANSYS are presented. The electronics interface will also be discussed.

 
TH5RFP057 Fast Horizontal e+ Instability Measurements in DAΦNE positron, feedback, dipole, electron 3585
 
  • A. Drago
    INFN/LNF, Frascati (Roma)
 
 

In the more than decennial history of DAΦNE, the Frascati e+/e- collider, the positron beam has always shown more difficulty to store high current than the e- beam. Given that the two rings are identical, many types of measurement have been tried to figure out the problem and to solve it, but eventually only one technique has presented a crucial utility: the modal grow rate measurement. In principle this method could be implemented using a commercial spectrum analyzer with the right software procedure inside. Nevertheless it is much easier and faster to record data by the bunch by bunch feedback diagnostics and to use for analyzing the offline feedback programs. A large campaign of data taking has been done in DAΦNE main rings during last fall. A comparison with grow rate records from previous years has point out clearly the difference with 2008 DAΦNE performance showing the way to solve the beam current limit. In particular, measurements have been done versus different machine conditions. Very fast horizontal instability present only in the e+ ring has been characterized showing linear behavior versus beam current. These data have been used to figure out the current limit problem.

 
TH5RFP063 Longitudinal Beam Dynamics in the HDSM at MAMI linac, synchrotron, microtron, injection 3594
 
  • M. Dehn, H. Euteneuer, A. Jankowiak
    IKP, Mainz
 
 

Funding: Work supported by DFG (CRC 443) and the German Federal State of Rheinland-Pfalz.


The 1.5GeV Harmonic Double Sided Microtron (HDSM)* as the fourth stage of the Mainz Microtron (MAMI) is now in routine operation for two and a half years**. Simulations predicted a wide range of applicable longitudinal parameters with which the machine can be run. Measurements of the longitudinal acceptance proved that. The reproducibility of different configurations is sufficient to support a fast and reliable set-up of the machine and to guarantee a stable long-term operation. But in order to optimise the configuration a reliable measurement of the phases and accelerating voltages in both linacs is essential. Each turn’s phase information is provided by low-Q-TM010 resonators at both linacs when operating the machine with 10ns diagnostic pulses. The HDSM’s four bending magnets are designed with a field gradient to compensate the vertical fringe defocusing. The decreasing field integral results in less synchronous energy gain per turn, automatically causing a change of the longitudinal phase. The calibration of the phase signals which in case of the RTMs could be easily done by exciting a synchrotron oscillation was improved to deliver precise phase data.


*K.-H. Kaiser et al., NIM A 593 (2008) 159 - 170, doi:10.{10}16/j.nima.2008.05.018
**A. Jankowiak et al., ID 2689, this conference

 
TH5RFP073 Test Results of the Luminosity Monitors for the LHC luminosity, electron, proton, booster 3612
 
  • A. Ratti, J.-F. Beche, J.M. Byrd, L.R. Doolittle, P.F. Manfredi, H.S. Matis, M.T. Monroy, J. Stiller, W.C. Turner, H. Yaver, T. stezelberger
    LBNL, Berkeley, California
  • E. Bravin
    CERN, Geneva
  • K.A. Drees
    BNL, Upton, Long Island, New York
 
 

The Luminosity Monitor for the LHC has been built at LBL and is going to be installed in the LHC in early 2009. The device designed for the high luminosity regions (ATLAS and CMS) is a gas ionization chamber, that is designed with the ability to resolve bunch by bunch luminosity as well as survive extreme levels of radiation. During the experimental R&D phase of its design, the prototype of this detector has been tested extensively in RHIC as well as in the SPS. Result of these experiments are shown here, with comments on the implications for early operations of the LHC.

 
TH5RFP079 Simulations of Picosecond Timing Using Large-Area Photodetectors electron, cathode, ion, radiation 3630
 
  • T.J. Roberts, R.J. Abrams, V. Ivanov
    Muons, Inc, Batavia
  • H.J. Frisch
    Enrico Fermi Institute, University of Chicago, Chicago, Illinois
 
 

Many measurements in particle and accelerator physics are limited by the time resolution with which individual particles can be detected. This includes particle identification via time-of-flight in major experiments like CDF at Fermilab and Atlas and CMS at the LHC, as well as the measurement of longitudinal variables in accelerator physics experiments. Large-scale systems, such as neutrino detectors, could be significantly improved by inexpensive, large-area photo detectors with resolutions of a few millimeters in space and a few picoseconds in time. Recent innovations make inexpensive, large-area detectors possible, with only minor compromises in spatial and time resolution. The G4beamline program [1] is one of the appropriate tools for simulation of low-energy physics processes. The set of specialized tools - MCPS [2], POISSON-2 [3] and Monte Carlo Simulator was used for numerical study of different photo multipliers.

 
TH5RFP082 Propagation Error Simulations Concerning the CLIC Active Prealignment linac, alignment, survey, emittance 3639
 
  • T. Touzé, H. Mainaud Durand, D.P. Missiaen
    CERN, Geneva
 
 

The CLIC components will have to be pre-aligned within a tolerance of 10 microns over a sliding window of 200m all along the linacs, before injecting the first beam. Such tolerance is about 30 times more demanding than for the existing machines as the SPS and LHC; it is a technical challenge and a key issue for the CLIC feasibility. In order to define the CLIC alignment strategy from the survey and beam dynamics point of view, simulations have been undertaken concerning the propagation error due to the measurement uncertainties of the pre-alignment systems. The uncertainties of measurement, taken as hypotheses for the simulations, are based on the data obtained on several dedicated facilities. This paper introduces the facilities and the latest results obtained, as well as the simulations performed.

 
TH5RFP086 Linear Collider Test Facility: ATF2 Final Focus Active Stabilisation Pertinence quadrupole, linear-collider, collider, ground-motion 3651
 
  • B. Bolzon, A. Jeremie
    IN2P3-LAPP, Annecy-le-Vieux
  • P. Bambade
    KEK, Ibaraki
  • Y. Renier
    LAL, Orsay
  • A. Seryi
    SLAC, Menlo Park, California
 
 

Funding: Work supported by the Agence Nationale de la Recherche of the French Ministry of Research (Programme Blanc, Project ATF2-IN2P3-KEK, contract ANR-06-BLAN-0027).


CLIC is one of the current projects of linear colliders. Achieving a vertical beam size of 1 nm at the Interaction Point (IP) with several nanometers of fast ground motion imposes an active stabilization of final doublet magnets (FD) at a tenth of nm above 4Hz. ATF2 is a test facility for linear colliders whose first aim is to have a vertical beam size of 37nm. Relative motion tolerance between FD and the IP is of 7nm above 0.1Hz. Because ground motion is coherent between these two elements, they were fixed to the floor so that they move in a coherent way. Investigations are going on to have in 2011 a useful active stabilization for ATF2 in order to use it as a CLIC prototype. Parameters of a 2D ground motion generator were fitted on measurements to reproduce spatial and temporal spectra, so it can be used for ATF2 simulations. Thus, we evaluated the ideal response function that an active stabilization FD system would need to have to improve on the present ATF2 system. Because ground motion coherence is lost with upstream magnets, we simulated the integrated vibrations at the IP to evaluate the usefulness of their stabilization. These results were validated with measurements.

 
TH5RFP091 Latest Data from the Linear Collider Alignment Survey Project (LiCAS) alignment, survey, laser, linear-collider 3666
 
  • A. Reichold, C. Uribe Estrada, D. Urner, S.Q. Yang
    OXFORDphysics, Oxford, Oxon
  • P.J. Brockill, J. Dale, M. Jones, G.R. Moss, R. Wastie
    JAI, Oxford
  • M. Schlösser
    DESY, Hamburg
 
 

Funding: work supported by STFC in the LC-ABD collaboration and by the Commission of the European Community, 6th Framework Programme, Structuring the European Research Area, contract number RIDS-011899


The Linear Collider Alignment and Survey group has completed experiments with a prototype robotic survey train for the ILC called the RTRS (Rapid Tunnel Reference Surveyor). Calibration of the RTRS is the most difficult part of data analysis, involving advanced mathematical methods to obtain constraint independent calibration parameters and errors. We show how sub-system data analysis provides input errors for the calibration process. We present the mathematical formalism used and results from the calibration of one of the three cars.

 
TH6PFP002 Beam Dynamics Simulations for CLIC Drive Beam Accelerator lattice, linac, quadrupole, wakefield 3690
 
  • A. Aksoy, O. Yavas
    Ankara University, Faculty of Engineering, Tandogan, Ankara
  • D. Schulte
    CERN, Geneva
 
 

Funding: Turkish Atomic Energy Authority


CLIC study aims at a center-of-mass energy for electron-positron collisions of 3TeV using room temperature accelerating structures at high frequency (12GHz) which are likely to achieve 100 MV/m gradient. Due to conventional high frequency RF sources do not provide sufficient RF power for 100MV/m gradient, CLIC relies upon a two-beam-acceleration concept: The 12GHz RF power is generated by a high current electron beam (Drive Beam) running parallel to the main beam with deceleration in special Power Extraction Structures (PETS) and the generated RF power is transferred to the main beam. In order to obtain very high RF power at 12GHz frequency, injected beam into PETS should have 2.37GeV energy, 101A pulse current and pulse length around 240ns. Drive beam accelerator (DBA) accelerates the beam up to 2.37GeV in almost fully-loaded structures and the pulse after DBA contains more than 70000 bunches, has a length around 140μs and 4.2A pulse current. After some modifications in delay loop and in combiner rings the beam has 101A pulse current and 240ns pulse length. In this study simulations of some transverse beam parameters for different options for the lattice of the DBA are presented.

 
TH6PFP004 Search for Nonlinear Beam Dynamics Causes of Lifetime Reduction at the APS Storage Ring sextupole, lattice, optics, power-supply 3696
 
  • L. Emery, M. Borland, V. Sajaev, A. Xiao
    ANL, Argonne
 
 

Funding: This work was supported by U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CHlI357.


During an operating period in which a sextupole unknowingly connected with the wrong polarity resulted in reduced beam lifetime, a list of machine physics experiments and simulations were developed to identify possible gradient errors of one or more sextupole magnets. We tried tune dependence on orbit, response matrix measurements at different momenta, sector-wise chromaticity measurements, empirical search with sextupole harmonics, and guidance from tracking simulations. The practicality of each will be discussed.

 
TH6PFP007 Simulation of Linear Lattice Correction and Coupling Correction of an Energy-Recovery Linac Designed for an APS Upgrade lattice, quadrupole, sextupole, optics 3705
 
  • V. Sajaev
    ANL, Argonne
 
 

Funding: Work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


An energy recovery linac (ERL) is one of the candidates for an upgrade of the Advanced Photon Source (APS). In addition to the APS ring and full-energy linac, our design also includes a large turn-around arc that could accommodate new x-ray beamlines as well. In total, the beam trajectory length would be close to 3 km. The ERL lattice has strong focusing to limit emittance growth, and it includes strong sextupoles to keep beam energy spread under control and minimize beam losses. As in storage rings, trajectory errors in sextupoles will result in lattice perturbations that would affect delivered x-ray beam properties. In storage rings, the response matrix fit method is widely used to measure and correct linear lattice errors. Here, we explore the application of the method to the linear lattice correction and coupling correction of an ERL.

 
TH6PFP017 Simulations on the AGS Horizontal Tune Jump Mechanism resonance, emittance, lattice, polarization 3735
 
  • F. Lin, H. Huang, A.U. Luccio, T. Roser
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


A new horizontal tune jump mechanism has been proposed to overcome the horizontal intrinsic resonances and preserve the polarization of the proton beam in the AGS during the energy ramp. An adiabatic change of the AGS lattice is needed to avoid the emittance growth in both horizontal and vertical motion, as the emittance growth can deteriorate the polarization of the proton beam. Two critical questions are necessary to be answered: how fast can the lattice be changed and how much emittance growth can be tolerated from both optics and polarization points of view? Preliminary simulations, using a realistic AGS lattice and acceleration rate, have been carried out to give a first glance of this mechanism. Several different conditions are presented in this paper.

 
TH6PFP028 Model Independent Analysis with Coupled Beam Motion coupling, dipole, betatron, resonance 3759
 
  • M.G. Billing, M.J. Forster, H.A. Williams
    CLASSE, Ithaca, New York
 
 

This paper describes the results of measurements compared with the analysis of errors for a method of determining accelerator Twiss and coupling parameters from the singular value decomposition of beam position monitor data, taken on a turn-by-turn basis for a storage ring in fully coupled transverse beam coordinates. Using the transversely coupled-coordinate formalism described by Billing et al*, the measurement technique expands on the work of Wang et al**, which describes the SVD of the same data under the assumptions of no transverse coupling of the beam parameters. This particular method of data analysis requires a set of BPM measurements, taken when the beam is resonantly excited in each of its two dipole, betatron normal-modes of oscillation


*M. Billing, et al, to be published in Phys. Rev. S T – Accel Beams
**C. Wang, et al, Phys. Rev. S T – Accel Beams 6, 104001 (2003)

 
TH6PFP042 The 4 GeV H- Beam Transfer Line from the SPL to the PS2 quadrupole, linac, beam-losses, injection 3799
 
  • C. Heßler, M. Eshraqi, B. Goddard, A.M. Lombardi, M. Meddahi
    CERN, Geneva
 
 

The proposed new CERN injector chain LINAC4, SPL, PS2 will require the construction of new beam transfer lines. A preliminary design has been performed for the 4 GeV SPL to PS2 H- transfer line. The constraints, beam parameters and geometry requirements are summarised and a possible layout proposed, together with the magnet specifications. First considerations on longitudinal beam dynamics and on beam loss limitations from H- lifetime are presented.

 
TH6PFP047 CLIC Main Beam Dynamics in the Ring to Main Linac Transport linac, wakefield, lattice, emittance 3814
 
  • F. Stulle, L. Rinolfi, D. Schulte
    CERN, Geneva
  • A. Ferrari
    Uppsala University, Uppsala
  • A. Latina
    Fermilab, Batavia
 
 

Prior to acceleration in the main linac, the particle beams created in the centrally located injector have to be transported to the outer ends of the CLIC site. This transport should not only preserve the beam quality but also shape, characterize and tune the phase space distribution to match the requirements at the entrance of the main linac. Hence, the performance of the transport downstream of the damping rings up to the main linac, the so called RTML, is crucial for the overall performance of CLIC. The RTML consists of a variety of components like bunch compressors, accelerating cavities, spin rotators, collimators, diagnostics sections, feedback and feedforward systems, each serving a distinct function. We discuss the different parts of the RTML and the beam dynamics challenges connected to them. Their status is outlined and results of beam dynamics simulations are presented.

 
TH6PFP053 Linear and Nonlinear Beam Optics Studies in the SIS18 sextupole, optics, closed-orbit, lattice 3826
 
  • A.S. Parfenova, G. Franchetti
    GSI, Darmstadt
 
 

The GSI heavy ion synchrotron SIS18 will be used as a booster for the SIS100 synchrotron of the new FAIR facility. The linear corrections and measurements are a necessary step before the nonlinear field errors can be applied. A tune response to a change in a sextupole magnet strength for a certain Closed Orbit (CO) deformation is used to verify beta-functions of the SIS18 model at the location of the ring's sextupoles for chromaticity correction. The progress in development of Nonlinear Tune Response Matrix (NTRM) technique to diagnose nonlinear field components is presented.

 
TH6PFP054 Beam Dynamics Design of Debuncher System for J-PARC Linac Energy Upgrade linac, injection, cavity, controls 3829
 
  • M. Ikegami
    KEK, Ibaraki
  • T. Morishita, H. Sako
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  • T. Ohkawa
    MHI, Kobe
 
 

The output energy of J-PARC linac is planned to be upgraded from 181 MeV to 400 MeV by adding an ACS (Annular Coupled Structure linac) section. The debuncher system for J-PARC linac is also replaced in this energy upgrade. The new debuncher system will consist of two 972-MHz debuncher cavities with the separate-function configuration. In this configuration, the momentum jitter is corrected with the first debuncher, whereas the momentum spread is controlled with the second debuncher. This configuration is advantageous in simplifying the tuning procedure, and it is also beneficial in reducing the nonlinear effects of the debuncher cavities. In this paper, the beam dynamics design of the debuncher system is presented with some simulation results.

 
TH6PFP059 Beam Based Alignment Simulations and Measurements at the S-DALINAC cavity, emittance, alignment, SRF 3841
 
  • F. Hug, R. Eichhorn, A. Richter
    TU Darmstadt, Darmstadt
 
 

Funding: Supported by DFG via SFB 634


Operational Experience at the Darmstadt superconducting linac (S-DALINAC) showed unexpected effects on beam dynamics and beam quality. So operators could observe transverse beam deflections by changing phases of the SRF-Cavities. Furthermore there has been occurred a growth of normalized tranverse emittance by a factor of 2. The beam current in the S-DALINAC does not exceed 60 μA so space-charge effects could be eliminated to be the reason for the observations. In this work the effect of misalignment of the SRF-Cavities in the linac has been examined using beam-dynamic simulations with the tracking code GPT and measurements on the electron beam of the S-DALINAC. By measuring the transverse deflection of the beam by changes of the phases of the SRF-Cavities and comparing results with GPT-simulations a misalignment of the 5-cell capture cavity and first 20-cell cavity of several mm in both transverse directions could be found. This misalignment can explain transverse deflections as well as emittance growth. A correction of misalignment has been carried out using the described results. First measurements showed no more emittance growth and less beam-deflections by SRF-Cavities.

 
TH6PFP060 Touschek Background and Lifetime Studies for the SuperB Factory lattice, background, coupling, emittance 3844
 
  • M. Boscolo, M.E. Biagini, P. Raimondi
    INFN/LNF, Frascati (Roma)
  • E. Paoloni
    University of Pisa and INFN, Pisa
  • M.K. Sullivan
    SLAC, Menlo Park, California
 
 

The novel crab waist collision scheme under test at the DAΦNE Frascati phi-factory finds its natural application to the SuperB project, the asymmetric e+e- flavour factory at very high luminosity with low beam currents and reduced background possibly located at Tor Vergata University. The SuperB accelerator design requires a careful choice of beam parameters to reach a good trade-off between different effects. We present here simulation results for the Touschek backgrounds and lifetime obtained for the latest machine design. Distributions of the Touschek particle losses at the at the interaction region have been tracked into the detectors for further investigations. A set of collimators is foreseen to stop Touschek particles. Their position along the rings has also been studied, together with their shape optimization.

 
TH6PFP066 The Correction of Linear Lattice Gradient Errors Using an AC Dipole quadrupole, betatron, optics, dipole 3859
 
  • G. Wang, M. Bai, V. Litvinenko, T. Satogata
    BNL, Upton, Long Island, New York
 
 

Funding: Department of Energy


Precise measurements of optics from coherent betatron oscillations driven by ac dipoles have been demonstrated at RHIC and the Tevatron. For RHIC, the observed rms beta-beat is about 10%. Reduction of beta-beating is an essential component of performance optimization at high energy colliders. A scheme of optics correction was developed and tested in the RHIC 2008 run, using ac dipole optics for measurement and a few adjustable trim quadrupoles for correction. In this scheme, we first calculate the phase response matrix from the measured phase advance, and then apply a singular value decomposition (SVD) algorithm to the phase response matrix to find correction quadrupole strengths. We present both simulation and some preliminary experimental results of this correction.

 
TH6PFP075 Linear and Non-Linear Optics Measurements at SOLEIL undulator, resonance, storage-ring, optics 3877
 
  • R. Tomás, M. Aiba, G. Vanbavinckhove
    CERN, Geneva
  • A. Nadji, L.S. Nadolski, M.-A. Tordeux
    SOLEIL, Gif-sur-Yvette
 
 

The successful correction of non-linear resonances in DIAMOND using the BPM turn-by-turn data has motivated testing this approach in SOLEIL in collaboration with CERN. We report on the first experiences towards the correction of non-linear resonances in SOLEIL.

 
TH6PFP077 Automating the Computation of Quadrupole Transfer Maps and Matrices Utilizing Electromagnetic Field Solutions quadrupole, permanent-magnet, optics, beam-transport 3883
 
  • G.H. Gillespie, W. Hill
    G.H. Gillespie Associates, Inc., Del Mar, California
  • J.F. DeFord, B. Held
    STAAR/AWR Corporation, Mequon
 
 

Funding: Work at G. H. Gillespie Associates, Inc. funded by the U.S. Department of Energy SBIR grant number DE-FG02-05ER84360


An automated procedure for the calculation of particle transfer maps using computed magnetic field data has been developed for several types of magnetic quadrupoles. The Automated Transfer Map Generator (ATMG) software used for these calculations combines the Analyst program and specialized modules of the Particle Beam Optics Laboratory (PBO Lab). Analyst's scripted solids capability is used to develop models of different magnet concepts. The geometry and material attributes for a given magnet concept are encapsulated by a small number of magnet parameters. Quadrupoles of the same basic concept can be simulated by using different values for the magnet parameters. The three-dimensional magnetic field solver (MS3p) of the Analyst program is used to obtain the fields. New PBO Lab modules are used to automate the field computation, and then calculate the transfer maps and matrices through third-order using the Venturini-Dragt method. Examples for three different types of magnetic quadrupole lenses are presented: electromagnetic air-core, electromagnetic iron-core, and rare-earth permanent magnet quadrupoles.

 
TH6PFP079 Study of Integer Betatron Resonance Crossing in Scaling FFAG Accelerator resonance, betatron, acceleration, closed-orbit 3889
 
  • Y. Mori
    KEK, Ibaraki
  • Y. Ishi, Y. Kuriyama, A. Osanai, T. Uesugi
    KURRI, Osaka
 
 

Crossing of integer resonance in scaling FFAG accelerator has been studied experimentally with the injector of 150MeV FFAG complex at Kyoto University Research Reactor Institute (KURRI). The results were analyzed based on harmonic oscillator model and compared with beam tracking simulations.

 
TH6PFP084 Experimental Frequency Map Analysis Using Multiple BPMs damping, closed-orbit, lattice, storage-ring 3898
 
  • C. Steier, L. Yang
    LBNL, Berkeley, California
 
 

Funding: This work was supported by the Director, Office of Science, U. S. Department of Energy under Contract No. DE-AC02-05CH11231.


Frequency map analysis is being widely used, nowadays, both in simulations to design or improve accelerator lattices, as well as in experiments to study the transverse nonlinear dynamics in accelerators. A significant challenge to the use of frequency map analysis in experiments is the usually very fast decoherence of transverse oscillations, caused by the large nonlinearities of state-of-the-art lattices. Due to the decoherence, the center of mass oscillations of bunches often disappear in less than 100 turns. A potential way to get around this limitation is the use of multiple BPMs distributed (symetrically) around the storage ring. The presentation will describe the challenges multi-BPM frequency map analysis poses as well as initial results using the ALS.

 
TH6PFP085 Beam Dynamics Studies for the FRIB Driver Linac linac, cavity, ion, emittance 3901
 
  • Q. Zhao, M. Doleans, F. Marti, T.P. Wangler, X. Wu, R.C. York
    NSCL, East Lansing, Michigan
  • J. Qiang
    LBNL, Berkeley, California
 
 

Funding: U.S. Department of Energy


A driver linac has been designed for the proposed Facility for Rare Isotope Beam (FRIB) at Michigan State University. FRIB is a lower cost and reduced scope alternative to the Rare Isotope Accelerator (RIA) project. The superconducting driver linac will accelerate stable isotope beams to energies ≥200 MeV/u with a beam power up to 400 kW for the production of rare isotope beams. The driver linac consists of a front-end and two segments of superconducting linac connected by a charge stripping station. End-to-end beam simulation studies with high statistics have been performed using the RIAPMTQ and IMPACT codes on high performance parallel computers. These studies include misalignment of beam elements, rf amplitude and phase errors for cavities, and thickness variation of the stripping foil. Three-dimensional fields of the superconducting solenoids and cavities were used in the lattice evaluation. The simulation results demonstrate good driver linac performance. No uncontrolled beam losses were observed even for the challenging case of multiple charge state uranium beam acceleration. The beam dynamics issues will be discussed and the detail beam simulation results presented.

 
TH6PFP086 Single Particle Dynamics in the University of Maryland Electron Ring electron, lattice, space-charge, injection 3904
 
  • E.W. Nissen, B. Erdelyi
    Northern Illinois University, DeKalb, Illinois
  • S. Bernal, D.F. Sutter
    UMD, College Park, Maryland
 
 

We undertake a study of the single particle dynamics in a model of the University of Maryland Electron Ring. This accelerator uses a low energy electron beam to study the effects of space charge on beam dynamics. However, due to this low energy, other effects that are seldom taken into account in high energy accelerators become important to the single particle dynamics of the beam. The simulation is performed using COSY Infinity, which has the effects of the earth’s magnetic field added to it. When the simulated trajectories are compared to measured beam positions there is good agreement through the ninth section of the ring, at which point the difference between predicted and observed diverges. A method of calculating map elements corresponding to the measured data will be used to determine where issues with the ring that could cause these problems might be found.

 
TH6PFP090 Adiabatic Formation and Properties of a Quasi-Equilibrium Beam Distribution Mathced to a Periodic Focusing Lattice lattice, focusing, quadrupole, vacuum 3916
 
  • M. Dorf, R.C. Davidson, H. Qin, E. Startsev
    PPPL, Princeton, New Jersey
 
 

Funding: Research supported by the U.S. Department of Energy.


This paper reports on recent advances in the development of a numerical scheme for describing the quiescent loading of a quasi-equilibrium beam distribution matched to a periodic focusing lattice*. The scheme allows for matched-beam distribution formation by means of the adiabatic turn-on of the oscillating focusing field, and it is examined here for the cases of alternating-gradient quadrupole and periodic solenoidal lattices. Furthermore, various distributions are considered for the initial beam equilibrium. The self-similar evolution of the matched-beam density profile is observed for arbitrary choice of initial distribution function and lattice type. The numerical simulations are performed using the WARP particle-in-cell code.


* M.Dorf et al., Phys. Rev. ST Accel. Beams, submitted for publication(2009).

 
TH6PFP093 Nonlinear Beam Dynamics with Strong Damping and Space Charge in the CLIC Damping Ring damping, space-charge, resonance, emittance 3925
 
  • P.A. Piminov, E.B. Levichev, D.N. Shatilov
    BINP SB RAS, Novosibirsk
 
 

The beam is injected into the CLIC damping ring with the relatively large emittance and energy spread and then is damped to the extremely low phase volume. During the damping process the betatron frequency of each particle changes due to the space charge tune shift and nonlinear detuning produced by the chromatic sextupoles, wiggler nonlinear field components and by the space charge force. During the damping, the particle cross resonances, which can trap some fraction of the beam, cause the loss of intensity, the beam blow up and degrade the beam quality. In this paper we study the evolution of the beam distribution in time during the damping.

 
TH6PFP095 Linear and Non-Linear Model Optimisation for SOLEIL Storage Ring coupling, quadrupole, sextupole, lattice 3931
 
  • M.-A. Tordeux, P. Brunelle, A. Loulergue, A. Nadji, L.S. Nadolski
    SOLEIL, Gif-sur-Yvette
 
 

SOLEIL, the French 2.75 GeV third generation synchrotron light source, was commissioned 3 years ago. Thanks to beam-based measurements, the theoretical model of the storage ring lattice model has been improved. First, the quadrupole lengths in the hard edge model were finely tuned to get good agreement with the experimental measurements of betatron tunes for different optics. Second, the non-linear model was modified to better fit with beam-based on-momentum frequency map measurements. A thick sextupole model has been introduced in addition to the non-linear effect of the fringe field in quadrupoles. Simulated and measured tune shifts with transverse amplitudes are then compared. Finally a coupled machine model has been built thanks to crosstalk closed orbit acquisitions. A comparison with another model which is based on turn by turn beam position monitor data is presented. As a validation check, the coupling effect of the 10 m long HU640 undulator is evaluated through these coupled models.

 
TH6PFP096 Analytical Calculation of the Smear for Long-Range Beam-Beam Interactions emittance, resonance, betatron, luminosity 3934
 
  • D. Kaltchev
    TRIUMF, Vancouver
  • W. Herr
    CERN, Geneva
 
 

The Lie-algebraic method is used to develop generalized Courant-Snyder invariant in the presence of an arbitrary number of beam-beam collisions, head-on or long-range, in a storage ring collider. The invariant is obtained by concatenating nonlinear beam-beam maps in the horizontal plane and to first order in the beam-beam parameter. Tracking evidence is presented to illustrate that with LHC parameters the invariant is indeed preserved and can be used to predict the smear of horizontal emittance observed in tracking simulations. We discuss the limits of applicability of this model for realistic LHC collision schemes.

 
TH6PFP098 Studies of the nur=3/2 Resonance in the TRIUMF Cyclotron resonance, cyclotron, TRIUMF, extraction 3940
 
  • Y.-N. Rao, R.A. Baartman, G. Dutto, L.W. Root
    TRIUMF, Vancouver
 
 

Funding: TRIUMF receives funding via a contribution agreement through the National Research Council of Canada.


The TRIUMF cyclotron is 6-fold symmetric, but has a 3rd harmonic magnetic field gradient error. As well, there is a 3rd harmonic component generated from the beating of the primary harmonics with the 9th harmonic. Both can contribute and drive the nur=3/2 resonance. As a consequence, the radial phase space ellipses become stretched and mismatched; this introduces a radial modulation of beam density and thereby causes a sensitivity of the extracted current to, for example, small changes in rf voltage. The cyclotron has "harmonic" correction coils, but these were designed to generate a first harmonic, not a third harmonic. Their 6-fold symmetric layout can only generate a 3rd harmonic at one particular phase and so can only partially compensate for this resonance. For a complete compensation, the 6 pairs of this harmonic coil would have to shift in azimuth by ~30degr. This paper describes the simulations performed with COMA to study the effect of this resonance. Initial measurement results are also presented.

 
TH6REP011 Longitudinal Beam Diagnostics for the ILC Injectors and Bunch Compressors diagnostics, electron, linac, positron 3971
 
  • P. Piot, A. Bracke, V. Demir, T.J. Maxwell, M.M. Rihaoui
    Northern Illinois University, DeKalb, Illinois
  • C.-J. Jing
    Euclid TechLabs, LLC, Solon, Ohio
  • J.G. Power
    ANL, Argonne
 
 

Funding: This work is supported by the U.S. Department of Energy under contract no. DE-FG02-06ER41435 with Northern Illinois University.


We present a diagnostics suite and analyze techniques for setting up the longitudinal beam dynamics in ILC e- injectors and e+ and e- bunch compressors. Techniques to measure the first order moments and recover the first order longitudinal transfer map of the injector's intricate bunching scheme are presented. Coherent transition radiation diagnostics needed to measure and monitor the bunch length downstream of the ~5 GeV bunch compressor are investigated using a vector diffraction model.

 
TH6REP013 Measurement and Detailed Simulation of Beam Losses Caused by Thin Interception Devices (Wire Scanners, Scrapers) at SNS beam-losses, linac, neutron, radiation 3977
 
  • A.P. Zhukov
    ORNL, Oak Ridge, Tennessee
  • I. Nesterenko
    BINP SB RAS, Novosibirsk
 
 

Funding: ORNL/SNS is managed by UT-Battelle, LLC, for the U.S. Department of Energy under contract DE-AC05-00OR22725.


Conversion of BLM readings into number of lost particles is a challenging task. Any insertion device is a good mean to obtain a localized loss and obtain such conversion factor with direct measurement. Such a measurement serves as a good benchmark for Monte-Carlo simulation of radiation transport. We used wire scanners and scraper induced losses to perform analysis of BLM response to local loss. The paper also provides a technique to measure 0.1% of full beam charge being intercepted by scraper during 650kW production run extracting the useful signal from high noise (20 times higher than signal) environment

 
TH6REP014 A Simulation Based Thermal Analysis of a New Current Monitor at the PSI Proton Accelerator proton, target, quadrupole, monitoring 3979
 
  • Y. Lee, P.-A. Duperrex, D.C. Kiselev, U. Muller
    PSI, Villigen
 
 

The Paul Scherrer Institute (PSI) operates a high power proton accelerator for the research projects in physical and medical sciences. Currently, a proton beam current of 2mA with a beam power of 1.2MW is routinely used. In the future, the ring cyclotron with new cavities will make a proton beam current of 3mA possible. The enhanced beam power will generate higher thermal and mechanical loads to different accelerator components. In this paper, a simulation based study of a new current monitor designed to sustain the 3mA beam operation is presented. The monitor is located behind the second graphite target and exposed to scattered particles and their secondaries. The thermal energy deposition in the current monitor has been calculated by the Monte-Carlo particle transport code MARS. The calculated power source has been used for the the coupled flow, heat and radiation simulations, for the prediction of the operating temperature. The effect of the newly introduced water cooling system and the surface blackening has been analyzed by using CFX. The thermal properties of the monitor system have been measured by laboratory experiments, and a simulation validation study is presented.

 
TH6REP022 Beam Orbit Tilt Monitor Studies at ATF2 cavity, monitoring, target, coupling 3994
 
  • D. Okamoto
    RCNS, Sendai
  • Y. Honda
    KEK, Ibaraki
  • T. Sanuki
    Tohoku University, School of Scinece, Sendai
 
 

We have designed a beam orbit tilt monitor for stabilizing a beam orbit in ATF2. Once we can measure a beam orbit tilt angle with high precision at one point, we can relate this data with the beam position profile at the focal point. This monitor is composed of a single rectangular cavity and waveguides to extract the signal. This monitor can measure the beam orbit tilt with a single cavity. We extract the signal of one basic resonance mode from the cavity. This electric field mode is perpendicular to the nominal beam axis, and is excited by beam tilt. The magnitude of extracted signal gives us the beam tilt data. According to our simulation, the expected sensitivity is about 30 nrad.

 
TH6REP024 A Proposal of a Single Coupler Cavity Beam Position Monitor cavity, coupling, dipole, radio-frequency 4000
 
  • A. Lyapin
    UCL, London
  • S.T. Boogert
    Royal Holloway, University of London, Surrey
 
 

Cavity beam position monitors (CBPM) made a significant progress in the last 10 years with an entire nano-beamline relying on them being currently commissioned at ATF2 (KEK). The major improvement was the introduction of the mode selective coupling allowing for efficient rejection of unwanted monopole modes. We propose another step towards creating a simple and cost effective CBPM - a cavity using just one coupler (instead of 2 or even 4) to couple out both polarisations of the dipole mode. The x and y signals are then split in the mixing stage of the electronics, so that only one expensive high-frequency electronics front-end is used for both x and y. A very good separation of the x and y signals can be achieved with a reasonable performance mixer assembly. In this paper we present the concept and provide some simulation results proving this processing scheme.

 
TH6REP028 Development of the C-Band BPM System for ATF2 cavity, EPICS, extraction, controls 4009
 
  • S. Molloy, R. Ainsworth, S.T. Boogert, G.E. Boorman
    Royal Holloway, University of London, Surrey
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • Y. Honda, T. Tauchi, N. Terunuma
    KEK, Ibaraki
  • A. Lyapin, B. Maiheu, M. Wing
    UCL, London
  • D.J. McCormick, J. Nelson, G.R. White
    SLAC, Menlo Park, California
  • S. Shin
    Fermilab, Batavia
  • D.R. Ward
    University of Cambridge, Cambridge
 
 

The ATF2 international collaboration is intending to demonstrate nanometre beam sizes required for the future Linear Colliders. An essential part of the beam diagnostics needed to achieve that goal is the high resolution cavity beam position monitors (BPMs). In this paper we report on the C-band system consisting of 32 BPMs spread over the whole length of the new ATF2 extraction beamline. We discuss the design of the BPMs and electronics, main features of the DAQ system, and the first operational experience with these BPMs.

 
TH6REP036 LCLS Stripline BPM System Commissioning controls, linac, diagnostics, low-level-rf 4027
 
  • S.R. Smith, R.G. Johnson, E. A. Medvedko
    SLAC, Menlo Park, California
 
 

Funding: Work supported by U.S. Department of Energy under Contract No. DE-AC02-76SF00515.


The Linac Coherent Light Source (LCLS) begins operation this year with 83 new stripline beam position monitor (BPM) processors. System requirements include several-micron position resolution for single-bunch beam charge of 200 pC. We describe the processing scheme, system specifications, commissioning experience, and performance measurements.

 
TH6REP049 Advanced Longitudinal Diagnostic for Single-Spike Operation at the SPARC FEL diagnostics, FEL, laser, alignment 4063
 
  • G. Marcus, G. Andonian, A. Fukasawa, P. Musumeci, S. Reiche, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • M. Ferrario, L. Palumbo
    INFN/LNF, Frascati (Roma)
  • L. Giannessi
    ENEA C.R. Frascati, Frascati (Roma)
 
 

It has been suggested that an ultra-short, very low charge beam be used to drive short wavelength single-spike operation at the SPARC FEL. This paper explores the development and construction of a longitudinal diagnostic capable of completely characterizing the radiation based on the Frequency-Resolved Optical Gating (FROG) technique. In particular, this paper explores a new geometry based on a Transient-Grating (TG) nonlinear interaction and includes studies of start to end simulations for pulses at the SPARC facility using GENESIS and reconstructed using the FROG algorithm. The experimental design, construction and initial testing of the diagnostic are also discussed.

 
TH6REP075 Design and Performance of Intra-Train Feedback Systems at ATF2 feedback, kicker, controls, extraction 4129
 
  • J. Resta-López, P. Burrows
    JAI, Oxford
 
 

The major goals of the final focus test beam line facility ATF2 are to provide electron beams with a few tens nanometer beam sizes and beam stability control at the nanometer level. In order to achieve such a level of stability beam based feedback systems are necessary at different timescales to correct static and dynamic effects. In particular, we present the design of intra-train feedback systems to correct the impact of fast jitter sources. We study a bunch-to-bunch feedback system to be installed at the extraction line to combat the ring extraction transverse jitters. In addition, we design a bunch-to-bunch feedback system at the interaction point for correction of position jitter due to the fast vibration of the magnets in the final focus. Optimum feedback software algorithms are discussed and simulation results are presented.

 
TH6REP078 Feedback Techniques and SPS Ecloud Instabilities – Design Estimates feedback, controls, pick-up, electron 4135
 
  • J.D. Fox, T. Mastorides, G. Ndabashimiye, C.H. Rivetta, D. Van Winkle
    SLAC, Menlo Park, California
  • J.M. Byrd, J.-L. Vay
    LBNL, Berkeley, California
  • R. De Maria
    BNL, Upton, Long Island, New York
  • W. Höfle, G. Rumolo
    CERN, Geneva
 
 

Funding: Work supported by Department of Energy contract DE–AC03–76SF00515 and the US LARP program.


The SPS at high intensities exhibits transverse single-bunch instabilities with signatures consistent with an Ecloud driven instability. While the SPS has a coupled-bunch transverse feedback system, control of Ecloud-driven motion requires a much wider control bandwidth capable of sensing and controlling motion within each bunched beam. This paper draws beam dynamics data from the measurements and simulations of this SPS instability, and develops initial performance requirements for a feedback system with 2-4 GS/sec sampling rates to damp Ecloud-driven transverse motion in the SPS at intensities desired for high-current LHC operation. Requirements for pickups, kickers and signal processing architectures are presented. Initial lab measurements of proof-of-principle lab model prototypes are presented for the wideband kicker driver signal functions.

 
TH6REP081 Calculation and Simulation of the Stripline Kicker Used in HLS kicker, feedback, impedance, pick-up 4144
 
  • Y.B. Chen, L. Liu, M. Meng, B. Sun, J.H. Wang, L. Wang, Y.L. Yang, Z.R. Zhou
    USTC/NSRL, Hefei, Anhui
 
 

A bunch-by-bunch analogue transverse feedback system at the Hefei Light Source (HLS) is to cure the resistive wall instability and the transverse coupled bunch instabilities. The kicker of the feedback system has four 21-cm-long electrodes of stripline type mounted in a skew 45°. Calculation and Simulation of the transverse kicker are shown.

 
TH6REP087 Firmware Development for SNS New Timing Master neutron, target, HOM, controls 4162
 
  • R. Štefanič, J. Dedič
    Cosylab, Ljubljana
  • D. Curry
    ORNL RAD, Oak Ridge, Tennessee
  • D.H. Thompson
    ORNL, Oak Ridge, Tennessee
 
 

Funding: This manuscript has been authored by UT-Battelle, LLC, under contract DE-AC05-00OR22725 with the U.S. Department of Energy.


Implementation of a timing system master device is a complicated task, since a lot of details have to be taken into account even once the architecture decisions have been laid down. At SNS/ORNL timing master controller is being upgraded in collaboration with Cosylab and this paper focuses on some details of its implementation. New timing system master device is based on agile FPGA circuitry and the main focus of this paper is its firmware implementation. Provided are implementation details for event distribution supporting multiple event sources and priorities. Discussed are mechanisms, ensuring deterministic behavior, different methods of encoding that have been employed, and host-independent distribution of time stamp frames. The concept of the super-cycle is explained and its implementation is laid down. Taken into account that implementation for such a complex device involves extensive testing, paper provides insight into verification it was applied. Advantages of the SystemC based test-benches over traditional VHDL-only verification are discussed.

 
TH6REP101 Timing Jitter Characterization at the NSLS SDL laser, electron, linac, gun 4189
 
  • H.J. Qian, C.-X. Tang
    TUB, Beijing
  • Y. Hidaka, J.B. Murphy, B. Podobedov, H.J. Qian, S. Seletskiy, Y. Shen, X.J. Wang, X. Yang
    BNL, Upton, Long Island, New York
 
 

Synchronization between a laser system and an electron beam plays a critical role in photoinjector operation, pump-probe experiments and many other applications. Here we report two novel experimental techniques for measuring the laser to RF timing jitter in a photoinjector, and e-beam arrival timing jitter after a magnetic chicane bunch compressor. The laser to RF timing jitter was characterized by observing the electron beam charge fluctuation through the Schottky effect. This technique was used to characterize the SDL photoinjector laser to RF timing jitter as a function of the temperature fluctuation in the laser room, and we have shown the resolution of this technique is ~100 fs. A stripline beam position monitor (BPM) located down stream of the compressor will be used to investigate the e-beam arrival timing jitter after a magnetic chicane bunch compressor; the outputs of the stripline BPM can be used to measure the arrival timing jitter by mixing them with a RF reference signal. The effect of the chicane on the arrival time jitters will be studied for the first time using this technique.

 
TH6REP102 Electro-Optic Sampling of Low Charge Low Energy Relativistic Electron Bunches at Pegasus Laboratory laser, electron, polarization, monitoring 4192
 
  • C.M. Scoby, M.S. Gutierrez, J.T. Moody, P. Musumeci
    UCLA, Los Angeles, California
 
 

Funding: Office of Naval Research (US) Grant No. N000140711174


Electro-optic sampling (EOS) has been developed as a timing monitor at Pegasus photoinjector laboratory for 100-fs electron bunches. A geometrically simple 2-dimensional spatially encoding scheme is used to measure time-of-arrival (TOA) of these ultrashort electron bunches in a 20 ps window down to < 50 fs resolution. The setup described here has successfully observed EOS signals for low energy (~4 MeV) and low charge (< 10 pC) bunches, both parameters being lower than electro-optic TOA monitors currently used in other labs. Experimental 2-d EOS images are compared to particle-in-cell plasma simulations (OOPIC) of electron bunch transient electric fields in ZnTe and to theoretical field propagation in dielectric crystals.

 
FR2PBI01 Advances in Impedance Theory impedance, wakefield, electromagnetic-fields, FEL 4270
 
  • G.V. Stupakov
    SLAC, Menlo Park, California
 
 

Funding: Work supported by US DOE contracts DE-AC03-76SF00515.


A remarkable progress over the last decade in development of computer codes significantly advanced our capabilities in calculation of wakefields and impedances for accelerators. There are however a number of practical problems that, when approached numerically, require a huge mesh, and hence memory, or an extraordinary CPU power, or both. One class of such problems is related to wakes of ultra short bunches, typical for many next generation electron/positron accelerators and photon sources. Another class is represented by long shallow collimators and tapers, often with non round cross sections. The numerical difficulties with these problems can be traced to a small parameter in the system, such as, e.g., a ratio of the bunch length to the length of a taper. It is remarkably, however, that the same small parameter often allows developing approximate analytical methods that provide a simplified solution to the impedance problem. In this paper, we review recent results in the analytical theory of wakefields, which include calculation of the wakes of very short bunches, long transitions and some special cases of the resistive wall impedance.

 

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FR2PBI02 Gravitational Instability of a Nonrotating Galaxy damping, impedance, collective-effects, wakefield 4275
 
  • A. Chao
    SLAC, Menlo Park, California
 
 

Funding: This work was supported by Department of Energy contract DE-AC02-76SF00515.


Gravitational instability of a star distribution in a galaxy is a well-known phenomenon in astrophysics. This problem can be analyzed using the standard tools developed in accelerator physics for analyzing the onset of beam instability and loss of Landau damping. An attempt is made here for a nonrotating galaxy. Predictions for the maximum stable galaxy size are in remarkable agreement with observations.

 

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FR5PFP004 Orbit Reconstruction, Correction, Stabilization and Monitoring in the ATF2 Extraction Line monitoring, emittance, quadrupole, extraction 4311
 
  • Y. Renier, P. Bambade
    LAL, Orsay
  • B. Bolzon
    IN2P3-LAPP, Annecy-le-Vieux
  • T. Okugi
    KEK, Ibaraki
  • A. Scarfe
    UMAN, Manchester
  • G.R. White
    SLAC, Menlo Park, California
 
 

Funding: CNRS/IN2P3 ANR (Programme Blanc, Project ATF2-IN2P3-KEK, contract ANR-06-BLAN-0027)


The orbit in the ATF2 extraction line has to be accurately controlled to allow orbit and optics corrections to work well downstream. The Final Focus section contains points with large beta function values which amplify incoming beam jitter, and few correctors since the steering is performed using quadrupole movers, and so good orbit stability is required. It is also essential because some magnets are non-linear and can introduce position-dependent coupling of the motion between the two transverse planes. First experience monitoring the orbit in the extraction line during the ATF2 commissioning is described, along with a simulation of the planned steering algorithm.

 
FR5PFP014 Errors in Beam Emittance Measurement in a Transport Channel emittance, quadrupole, linac, linear-collider 4338
 
  • Y.K. Batygin
    NSCL, East Lansing, Michigan
  • M. Woodley
    SLAC, Menlo Park, California
 
 

Determination of exact values of beam emittance is important for future linear collider. Beam emittance measurements technique is based on measurement of beam sizes at several beam profile stations in a quadrupole channel shifted between each other by a specific value of phase advance of betatron oscillations. Four-dimensional beam emittance measuremenst requires determination of ten values of the beam σ-matrix, while two-dimensional beam emittance measurements scheme requires determination of six values of σ-matrix. Measurement procedure is sensitive to variation of beam sizes at the beam profile stations, which might result in unstable determination of beam emittance. Paper discusses errors of beam emittance measurements as a function of errors in beam size measurement. Regions of stable and unstable beam emittance measurements are determined.

 
FR5PFP015 An Achromatic Mass Separator Design for Ions from the EBIT Charge Breeder at the NSCL ion, injection, quadrupole, emittance 4341
 
  • M. Portillo, G. Bollen, S. Chouhan, O.K. Kester, G. Machicoane, J. Ottarson, S. Schwarz, A. Zeller
    NSCL, East Lansing, Michigan
 
 

Funding: This work was supported by Michigan State University and the National Science Foundation under grant PHY-0110253.


The NSCL at Michigan State University (MSU) is implementing a system called the ReA3 to reaccelerate rare isotope beams from projectile fragmentation to energies of about 3 MeV/u. The re-acceleration system uses an Electron Beam Ion Trap (EBIT) to provide a compact and cost efficient system. We discuss the design parameters for a m/q separator that is to be used to separate highly charged ions from an EBIT type charge breeder. The separator is designed to accept ions at 12 keV/u with mass to charge ratios in the range of m/q = 2.5 to 5 amu. The goal is to separate selected rare isotope species from any residual ions before injecting them into the ReA3 linear accelerator system. Using ray tracing simulations with SIMION*, as well as higher order map calculations with COSY INFINITY**, the performance of the separator has been evaluated in terms of the expected mass resolution and overall acceptance. The separator consists of a magnetic sector and a series of electrostatic devices to obtain a first order achromatic tune. For comparison, similar performance values will be derived as those for a similar separator constructed at REX-ISOLDE***.


*D.A. Dahl, Int. J. Mass Spectrom. Ion Processes 200, 3 (2000) .
**K. Makino and M. Berz, Nucl. Instr. and Meth. A 558, 346 (2005)
***R. Rao et. al., EPAC-98, Stockholm, Sweden, 2132-2134 (1998).

 
FR5PFP021 Plans and Progress towards Tuning the ATF2 Final Focus System to Obtain a 35nm IP Waist emittance, optics, sextupole, coupling 4353
 
  • G.R. White
    SLAC, Menlo Park, California
  • J.K. Jones
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • K. Kubo, S. Kuroda
    KEK, Ibaraki
  • Y. Renier
    LAL, Orsay
  • A. Scarfe
    UMAN, Manchester
  • R. Tomás
    CERN, Geneva
 
 

Funding: Work supported in part by Department of Energy Contract DE-AC02-76SF00515


Using a new extraction line currently being commissioned, the ATF2 experiment plans to test a novel compact final focus optics design using a local chromaticity correction scheme, such as could be used in future linear colliders*. Using a 1.3 GeV beam of ~30nm normalised vertical emittance extracted from the ATF damping ring, the primary goal is to achieve a vertical IP waist of 35nm. We discuss our planned strategy, implementation details and early experimental results for tuning the ATF2 beam to meet the primary goal. These optics require uniquely tight tolerances on some magnet strengths and positions, we discuss efforts to re-match the optics to meet these requirements using high-precision measurements of key magnet elements. We simulated in detail the tuning procedure using several algorithms and different code implementations for comparison from initial orbit establishment to final IP spot-size tuning. Through a Monte Carlo study of 100's of simulation seeds we find we can achieve a spot-size within 10% of the design optics value in at least 90% of cases. We also ran a simulation to study the long-term performance with the use of beam-based feedbacks.


*"ATF2 Proposal", ATF2 Collaboration (Boris Ivanovich Grishanov et al.)., KEK-REPORT-2005-2, Aug 23, 2005.

 
FR5PFP031 Possible Limitations in Coupling Correction Using Orbit Response Matrix Analysis quadrupole, emittance, coupling, optics 4375
 
  • K.G. Panagiotidis
    The University of Liverpool, Liverpool
  • K.G. Panagiotidis, A. Wolski
    Cockcroft Institute, Warrington, Cheshire
 
 

The specified vertical emittance for the ILC damping rings is 2 pm. A major objective for the Accelerator Test Facility (ATF) at KEK is to demonstrate reliable operation in this low emittance regime. LOCO is a tool for identifying optics errors in storage rings, based on fitting a lattice model to the measured closed orbit response matrix. This technique can be used to determine corrections to minimise vertical dispersion and betatron coupling, and hence reduce the vertical emittance. So far, efforts to apply LOCO to the ATF to achieve 2 pm vertical emittance have met with limited success. This paper presents the results of simulations aiming to identify possible limitations in the technique. We consider the effects of varying parameters controlling the fit of the lattice model to the measured data, and investigate possible degeneracies (e.g. between skew quadrupole strengths and tilts of the corrector magnets) that may limit the quality of the correction achievable using this technique.

 
FR5PFP035 6D Cooling Simulations for the Muon Collider cavity, emittance, solenoid, collider 4381
 
  • P. Snopok, G.G. Hanson
    UCR, Riverside, California
 
 

Funding: Work supported by the United States Department of Energy under Grant No. DE-FG02-07ER41487.


The RFOFO ring is considered to be one of the most promising six-dimensional cooling channels proposed for the future Muon Collider. It has a number of advantages over other cooling channels, but also certain drawbacks. The injection and extraction, the absorber overheating, and the bunch train length are among the main issues. A number of simulations of a possible solution to these problems, the RFOFO helix, commonly referred to as the Guggenheim channel, were carried out and their results are summarized. The issue of the RF breakdown in the magnetic field is addressed, and the preliminary results of the simulation of the lattice with magnetic coils in the irises of the RF cavities are presented.

 
FR5PFP038 Possible Emittance Growth due to Nonuniform Particle Distribution in Beams with Thermal Equilibrium Condition emittance, space-charge, lattice, plasma 4390
 
  • T. Kikuchi
    Nagaoka University of Technology, Nagaoka, Niigata
  • K. Horioka
    TIT, Yokohama
 
 

Possible emittance growth due to a nonuniform particle distribution can be analyzed with a thermal equilibrium state in various space-charge potential beams. The possible emittance growth is given by a function of a space-charge tune depression and a nonlinear field energy factor. The nonlinear field energy factor, which is determined by nonuniformity of a charge distribution, is estimated in the thermal equilibrium distribution on a cross-section in a beam. The nonlinear field energy factor changes with space-charge potential for the thermal equilibrium distribution. It is expected that the possible emittance growth will be decreased effectively to consider in the thermal equilibrium condition.

 
FR5PFP039 Verification of the AWA Photoinjector Beam Parameters Required for a Transverse-to-Longitudinal Emittance Exchange Experiment emittance, booster, laser, gun 4393
 
  • M.M. Rihaoui, D. Mihalcea, P. Piot
    Northern Illinois University, DeKalb, Illinois
  • W. Gai, J.G. Power
    ANL, Argonne
 
 

A transverse-to-longitudinal emittance exchange experiment is in preparation at the Argonne Wakefield Accelerator (AWA). The experiment aims at exchanging a low (< 5 mm-mrad) longitudinal emittance with a large (>15 mm-mrad) transverse horizontal emittance for a bunch charge of 100 pC. Achieving such emittance partitioning, though demonstrated via numerical simulations, is a challenging task and need to be experimentally verified. In this paper, we report emittance measurements of the beam in the transverse and longitudinal planes performed at 12 MeV. The measurements are compared with numerical simulations using Impact-T.

 
FR5PFP040 Measurement and Simulation of Space Charge Effects in a Multi-Beam Electron Bunch from an RF Photoinjector space-charge, laser, electron, gun 4396
 
  • M.M. Rihaoui, P. Piot
    Northern Illinois University, DeKalb, Illinois
  • W. Gai, J.G. Power, Z.M. Yusof
    ANL, Argonne
 
 

Funding: M.R. and P.P. was supported by the US DOE under Contracts No. DE-FG02-08ER41532 with NIU. W.G., J.P., and Z.Y. are supported by the U.S. DOE under Contract No. DE-AC02-06CH11357 with ANL.


We report on a new experimental study of the space charge effect in a space-charge-dominated multi-beam electron bunch. A 5 MeV electron bunch, consisting of a variable number of beamlets separated transversely, was generated in a photoinjector and propagated in a drift space. The collective interaction of these beamlets was studied for different experimental conditions. The experiment allowed the exploration of space charge effects and its comparison with three-dimensional particle-in-cell simulations. Our observations also suggest the possible use of a multi-beam configuration to tailor the transverse distribution of an electron beam.

 
FR5PFP041 ORBIT Benchmark of Extraction Kicker Instability Observed in SNS impedance, kicker, extraction, proton 4399
 
  • J.A. Holmes, S.M. Cousineau, V.V. Danilov
    ORNL, Oak Ridge, Tennessee
  • Z. Liu
    IUCF, Bloomington, Indiana
 
 

Funding: ORNL/SNS is managed by UT-Battelle, LLC, for the U.S. Department of Energy under contract DE-AC05-00OR22725.


During one of the high beam intensity runs in SNS, a coasting beam instability was observed in the ring when the beam was stored for 10000 turns. This instability was observed at an intensity of about 12 microcoulombs and was characterized by a frequency spectrum peaking at about 6 MHz. A likely cause of the instability is the impedance of the ring extraction kickers. We carry out here a detailed benchmark of the observed instability, uniting an analysis of the experimental data, a precise ORBIT Code tracking simulation, and a theoretical estimate of the observed beam instability.

 
FR5PFP043 Matching with Space Charge #2 space-charge, quadrupole, emittance, focusing 4405
 
  • S.B. van der Geer
    Pulsar Physics, Eindhoven
  • B.D. Muratori
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • M.J. de Loos, S.B. van der Geer
    TUE, Eindhoven
 
 

The required strengths of quadrupoles in a phase-space tomography section are significantly affected by the total charge per bunch. Finding settings at a high charge is challenging because of the non-linear nature of Coulomb interactions. This is further hindered by the inability to use thin-lens approximations and dependence on numerical simulations. Finally, one faces the problem that at some charge there simply is no solution at all. In this contribution we describe a simple procedure, implemented in the General Particle Tracer (GPT) code, which can be used to find optimal beamline settings in the presence of space-charge forces. The recipe 'transports' the settings for a zero-charge solution to those of the desired charge and it gives an indication what the maximum tolerable charge is.

 
FR5PFP044 Studies of Space Charge Loss Mechanisms Associated with Half Integer Resonance on the ISIS RCS resonance, space-charge, emittance, diagnostics 4408
 
  • C.M. Warsop, D.J. Adams, B. Jones, S.J. Payne, B.G. Pine, R.E. Williamson
    STFC/RAL/ISIS, Chilton, Didcot, Oxon
 
 

ISIS is the spallation neutron source at the Rutherford Appleton Laboratory in the UK. Operation centres on a 50 Hz proton synchrotron, which accelerates ~3·1013 ppp from 70 to 800 MeV, corresponding to beam powers of 0.2 MW. Beam loss imposes limits on operational intensity, and a main contributing mechanism is the action of half integer resonance under high space charge. The same loss mechanism is also a potential problem in ISIS upgrade scenarios involving either higher energy injection into the existing ring, or the addition of a new 3 GeV, high intensity RCS. Progress on particle in cell simulation studies investigating the effects of the driven coherent envelope motion, the associated parametric halo, along with implications of momentum spread, dispersion and longitudinal motion, is reported. Where possible, comparisons are made with relevant theoretical models. Closely related benchmarking work, experimental studies and plans are also summarised.

 
FR5PFP046 Longitudinal Dynamics Studies for ISIS Upgrades space-charge, longitudinal-dynamics, synchrotron, injection 4411
 
  • R.E. Williamson, B.G. Pine, C.M. Warsop
    STFC/RAL/ISIS, Chilton, Didcot, Oxon
 
 

ISIS is the pulsed neutron and muon source based at the Rutherford Appleton Laboratory in the UK. Operation is centred on a loss-limited 50 Hz proton synchrotron which accelerates ~3·1013 protons per pulse from 70 MeV to 800 MeV, corresponding to mean beam powers of 0.2 MW. A number of ISIS upgrades are currently under study. One option replaces the linac for higher energy injection into the existing ring, potentially increasing beam current through reduction in space charge. The other main option adds a new 3 GeV RCS, boosting the energy of the beam to provide higher beam power. For both these upgrade routes, longitudinal dynamics of the existing and proposed new rings play a crucial role in achieving high intensity with low loss. This paper outlines longitudinal beam dynamics studies in the rings for both these cases, including development of a new longitudinal space charge code, comparison of different algorithms and codes and treatment of the key beam dynamics issues for each case. The influence of non-space charge impedances is also considered.

 
FR5PFP047 Thermal Control of the Fermi@Elettra Accelerating Sections controls, cavity, linac, RF-structure 4414
 
  • C. Serpico, G. D'Auria, P. Delgiusto
    ELETTRA, Basovizza
 
 

Funding: "The work was supported in part by the Italian Ministry of University and Research under grant FIRB-RBAP045JF2 or grant FIRB-RBAP06AWK3 or grants FIRB-RBAP045JF2 and FIRB-RBAP06AWK3"


FERMI@Elettra is a FEL user facility under construction at Sincrotrone Trieste, Italy. It will use the existing normal conducting S-band Linac and seven accelerating sections received from CERN after the LIL decommissioning. Two additional new sections are also foreseen. The Linac repetition rate will be 10 Hz during the initial stage of operation, but it will be ramped up from 10 Hz to 50 Hz. Due to the higher RF power dissipation, the temperature distribution on the copper structure will reach higher values. RF heating will imply a thermal deformation of the accelerating cavities, both in the transversal and in the longitudinal direction. Since FERMI@Elettra has stringent requirements on phase stability, the length of the section must be kept as constant as possible. In this paper the thermo-mechanic behaviour of the accelerating sections is investigated and the results of the simulations are presented. Furthermore an algorithm has been developed to control the longitudinal deformation of the sections.

 
FR5PFP049 Effects of Transverse Physics on Nonlinear Evolution of Longitudinal Space-Charge Waves in Beams space-charge, solenoid, beam-losses, electron 4418
 
  • K. Tian
    JLAB, Newport News, Virginia
  • I. Haber, R.A. Kishek, P.G. O'Shea, M. Reiser
    UMD, College Park, Maryland
  • D. Stratakis
    BNL, Upton, Long Island, New York
 
 

Funding: This work is funded by the US Dept. of Energy Offices of High Energy Physics and High Energy Density Physics, and by the US Dept. of Defense Office of Naval Research and Joint Technology Office


Longitudinal space-charge waves can introduce energy perturbations into charge particle beams and degrade the beam quality, which is critical to many modern applications of particle accelerators. Although many longitudinal phenomena arising from small perturbations can be explained by a one-dimensional cold fluid theory, nonlinear behavior of space-charge waves observed in experiments has not been well understood. In this paper, we summarize our recent investigation by means of more detailed measurements and self-consistent simulations. Combining the numerical capability of a PIC code, WARP, with the detailed initial conditions measured by our newly developed time resolved 6-D phase space mapping technique, we are able to construct a self consistent model for studying the complex physics of longitudinal dynamics of space-charge dominated beams. Results from simulation studies suggest that the unexplained nonlinear behavior of space-charge waves may be due to transverse mismatch or misalignment of beams.

 
FR5PFP050 An Analytical Characterization of Initially Non-Homogeneous Matched Beams at Equilibrium emittance, focusing, background, resonance 4421
 
  • R.P. Nunes, F.B. Rizzato
    IF-UFRGS, Porto Alegre
 
 

Non-homogeneity is a characteristic naturally present in non-neutral beams. Recently, a set of works has been developed by us for the case of beams initially homogeneous, making possible that relevant macroscopic quantities such as the RMS radius and emittance could be determined at equilibrium as functions of characteristic parameters of beam phase-space and of initial conditions. The present work intends to investigate the influences of the initial inhomogeneity in the beam route to equilibrium. Through the same methodology introduced in the studies for the homogeneous beams, both emittance and beam envelope have been obtained as functions of the magnitude of the inhomogeneity and some additional parameters associated with geometry of beam phase-space. The results obtained with this investigation have proven to be useful not only to better understand the effects of inhomogeneity over beam dynamics but also to provide physical background to the investigations previously carried out for homogeneous beams.

 
FR5PFP052 On the Time Scale of Halo Formation in Homogeneous Mismatched Beams emittance, focusing, controls, collimation 4424
 
  • R.P. Nunes, F.B. Rizzato
    IF-UFRGS, Porto Alegre
 
 

Experiments and numerical simulations show that high-intensity beams composed by charged particles usually reach their final stationary state with a progressive populating of a spatial region external to its original border. This populating process occurs in such terms that beam spatial limits at equilibrium increase by an amount of two or three times its initial nominal size. This is known as halo in Beam Physics. In this way, this work intends to better understand the time scale of halo formation. The carried out investigation has shown that the time scale of halo formation in fact can be segmented in two different quantities, each one associated to distinct physical mechanisms. One is related with the initial non-homogeneity naturally present in such systems, and the other is a result of the initial beam envelope mismatch. This investigation seems to be useful to design more efficient collimation systems and/or non-linear control systems for the next generation high-power accelerators.

 
FR5PFP053 Centroid Dynamics of Magnetically Focused Intense Relativistic Charged Beams Surrounded by a Conducting Wall beam-transport, focusing 4427
 
  • R. Pakter, L.C. Martins, F.B. Rizzato
    IF-UFRGS, Porto Alegre
 
 

Funding: Work supported by CNPq, Brazil and the US-AFOSR under Grant No. FA9550-06-1-0345.


In this paper, we investigate the combined envelope-centroid dynamics of relativistic continuous charged beams transported through a uniform focusing field and surrounded by a conducting wall. For such beams, the conducting wall screens the electric field but allows magnetic field penetration, enhancing the induced charges effect on the beam transport. As a consequence, in contrast to the case of nonrelativistic beams where the walls are shown to have little effect*, relativistic beams may have their centroid motion severely affected, leading to limitations in the total current and area occupied by the beam inside the conductor. Self-consisted simulation are used to verify the findings.


*K. Fiuza, F. B. Rizzato, and R. Pakter, Phys. Plasmas, 13, 023101 (2006).

 
FR5PFP054 Relaxation of Intense Inhomogeneous Mismatched Charged Beams emittance, scattering, plasma, focusing 4428
 
  • F.B. Rizzato, A. Endler, R.P. Nunes, R. Pakter, E.G. Souza
    IF-UFRGS, Porto Alegre
 
 

Funding: CNPq, Brazil; AFOSR FA9550-06-1-0345, USA


In this work we analyze the dynamics of mismatched inhomogeneous beams of charged particles. Initial inhomogeneities lead to propagating density waves across the beam core, and the presence of density waves eventually results in density build up and particle scattering. Particle scattering off waves in the beam core and the presence of resonances due to envelope mismatches ultimately generate a halo of particles with concomitant emittance growth. Emittance growth directly indicates when the beam relaxes to its final stationary state, and the purpose of the present paper is to describe halo and emittance in terms of test particles moving under the action of the mismatched inhomogeneous beam. To this end we develop an average Lagrangian approach for the beam where both density and envelope mismatches are incorporated. Test particle results compare well with full simulations.

 
FR5PFP057 Beam Dynamics Simulations of the Velocity Bunching in a Superconducting Linac emittance, bunching, linac, gun 4437
 
  • A. Fukasawa, B.D. O'Shea, J.B. Rosenzweig
    UCLA, Los Angeles, California
 
 

The velocity bunching is a hot topic in normal conducting photoinjectors to generate high-brightness beams instead of magnetic chicanes in the low energy region. We apply this technique to the superconducting photoinjectors. The linac considered here consists of several 9-cell TESLA cavities, the standard 1.6-cell normal conducting RF gun is assumed, though. In the case of 1.1 nC injection, the peak current increases to 1 kA with 2.6 mm.mrad of the emittance. The peak current can be higher but the emittance becomes worse in that case, and vice versa. We discuss more details on the spot.

 
FR5PFP060 Modeling Acceleration of High Intensity Space-Charge-Dominated Beams acceleration, induction, emittance, space-charge 4446
 
  • K. Fiuza, B.L. Beaudoin, S. Bernal, I. Haber, R.A. Kishek, P.G. O'Shea, M. Reiser, D.F. Sutter
    UMD, College Park, Maryland
 
 

Funding: This work is funded by the US Dept. of Energy Offices of High Energy Physics and High Energy Density Physics, and by the US Dept. of Defense Office of Naval Research and Joint Technology Office.


Understanding the dynamics of the acceleration of high-intensity space-charge-dominated electron and ion beam is very important. Accelerating by steps a space-charge-dominated beam can be fundamentally different from beams at lower intensities, because at sufficiently high beam intensities the beam response to acceleration can drive to some unknown instabilities leading to a significant beam losses. This work analyses the acceleration of the University of Maryland Electron Ring (UMER) beam, i.e., high current, low-energy and space-charge-dominated electron beam which is applicable, on a scale basis, to a large class of other beam systems. We use the WARP particle-in-cell code to perform simulations that are compared with theoretical predictions and preliminary experimental results.

 
FR5PFP062 Halo Regeneration in Intense Charged Particle Beams collimation, space-charge, electron, focusing 4452
 
  • C. F. Papadopoulos, S. Bernal, I. Haber, R.A. Kishek, P.G. O'Shea, M. Reiser
    UMD, College Park, Maryland
 
 

Funding: This work is funded by the US Dept. of Energy Offices of High Energy Physics and High Energy Density Physics, and by the US Dept of Defense Office of Naval Research and Joint Technology Office.


Halo is one important limiting factor for the continuous and reliable operation of intense electron or ion beam facilities, such as FELs and spallation neutron sources. A halo population outside the core of the beam can lead to uncontrolled beam loss, electron cloud effects and activation of the beam pipe, as well as beam quality degradation. In this study, we focus on the issue of halo removal, by means of beam collimation, and subsequent halo regeneration. We compare the particle-core model of halo creation to accurate, self consistent particle-in-cell (PIC) simulations. We show that under certain conditions the halo is regenerated even after collimation. This can only be understood within the context of collective effects, particularly in the case of intense beams.

 
FR5PFP063 Coherent Phenomena over a Broad Range of Beam Intensities in the Electron Storage Ring UMER space-charge, electron, storage-ring, emittance 4455
 
  • D.F. Sutter, B.L. Beaudoin, S. Bernal, M. Cornacchia, K. Fiuza, I. Haber, R.A. Kishek, P.G. O'Shea, M. Reiser, C. Wu
    UMD, College Park, Maryland
 
 

Funding: *This work is funded by the US Dept. of Energy Offices of High Energy Physics and High Energy Density Physics, and by the US Dept. of Defense Office of Naval Research and Joint Technology Office


The University of Maryland Electron Ring (UMER) is designed for operation over a broad range of beam intensities, including those normally achieved only in linacs. This is possible thanks to a combination of low-energy (10 keV) electrons and a high density of magnetic quadrupoles (72 over an 11.5 m circumference) that allow operation from 0.5 mA to 100 mA; that is, from the emittance dominated to the highly space charge dominated regimes. We present results of basic centroid-motion characterization, including measurements of closed-orbit distortion, momentum compaction factor, and natural chromaticity and dispersion. These are compared with results from computer simulations employing the code ELEGANT. We discuss the techniques and challenges behind the measurements with fast beam-position and wall-current monitors, and also the special role of the background ambient magnetic field for beam steering.

 
FR5PFP065 The Object Oriented Parallel Accelerator Library (OPAL) space-charge, emittance, cathode, synchrotron 4461
 
  • A. Adelmann, Y. Ineichen, C. Kraus, T. Schietinger
    PSI, Villigen
  • S.J. Russell
    LANL, Los Alamos, New Mexico
  • J.J. Yang
    CIAE, Beijing
 
 

OPAL (Object Oriented Parallel Accelerator Library) is a tool for charged-particle optics in accelerator structures and beam lines including 3D space charge, short range wake-fields and a 1D coherent synchrotron radiation. Built from first principles as a parallel application, OPAL admits simulations of any scale, from the laptop to the largest HPC clusters available today. Simulations, in particular HPC (High Performance Computing) simulations, form the third pillar of science, complementing theory and experiment. In this paper we present numerical and HPC capabilities such as fast direct and iterative solvers together with timings up to several thousands of processors. The application of OPAL to our PSI-XFEL project as well as to the ongoing high power cyclotron upgrade will demonstrate OPAL's capabilities applied to ongoing projects at PSI. Plans for future developments will be discussed.

 
FR5PFP066 A User-Friendly Code to Model Radiation of High Brightness Beams radiation, lattice, diagnostics, brightness 4464
 
  • G. Andonian, M. Ruelas
    RadiaBeam, Marina del Rey
  • S. Reiche
    UCLA, Los Angeles, California
 
 

The accelerator community has many codes that model beams and emitted radiation. Many of these codes are specialized and often, as in start-to-end simulations, multiple codes are employed in subsequent fashion. One of the most important goals of simulations is to accurately model beam parameters and compare results to those obtained from real laboratory diagnostics. This paper describes the development of a user-friendly code that models the coherent radiation of high brightness beams, with a heavy emphasis on simulation of observables via laboratory diagnostics.

 
FR5PFP068 Wakefield Simulation of CLIC PETS Structure Using Parallel 3D Finite Element Time-Domain Solver T3P wakefield, impedance, damping, radio-frequency 4467
 
  • A.E. Candel, A.C. Kabel, K. Ko, L. Lee, Z. Li, C.-K. Ng, G.L. Schussman
    SLAC, Menlo Park, California
  • I. Syratchev
    CERN, Geneva
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


In recent years, SLAC's Advanced Computations Department (ACD) has developed the parallel 3D Finite Element electromagnetic time-domain code T3P. Higher-order Finite Element methods on conformal unstructured meshes and massively parallel processing allow unprecedented simulation accuracy for wakefield computations and simulations of transient effects in realistic accelerator structures. Applications include simulation of wakefield damping in the Compact Linear Collider (CLIC) Power Extraction and Transfer Structure (PETS).

 
FR5PFP069 Parallel 3D Finite Element Particle-in-Cell Simulations with Pic3P gun, space-charge, emittance, SRF 4470
 
  • A.E. Candel, A.C. Kabel, K. Ko, L. Lee, Z. Li, C.-K. Ng, G.L. Schussman
    SLAC, Menlo Park, California
  • I. Ben-Zvi, J. Kewisch
    BNL, Upton, Long Island, New York
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


SLAC's Advanced Computations Department (ACD) has developed the parallel 3D Finite Element electromagnetic Particle-In-Cell code Pic3P. Designed for simulations of beam-cavity interactions dominated by space charge effects, Pic3P solves the complete set of Maxwell-Lorentz equations self-consistently and includes space-charge, retardation and boundary effects from first principles. Higher-order Finite Element methods with adaptive refinement on conformal unstructured meshes lead to highly efficient use of computational resources. Massively parallel processing with dynamic load balancing enables large-scale modeling of photoinjectors with unprecedented accuracy, aiding the design and operation of next-generation accelerator facilities. Applications include the LCLS RF gun and the BNL polarized SRF gun.

 
FR5PFP071 Thermal Analysis of SCRF Cavity Couplers Using Parallel Multiphysics Tool TEM3P cavity, vacuum, HOM, cryogenics 4473
 
  • V. Akcelik, K. Ko, L. Lee, Z. Li, C.-K. Ng
    SLAC, Menlo Park, California
  • G. Cheng, R.A. Rimmer, H. Wang
    JLAB, Newport News, Virginia
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


SLAC has developed a multi-physics simulation code TEM3P for simulating integrated effects of electromagnetic, thermal and structural effects. TEM3P shares the same finite element infrastructure with EM finite elements codes developed at SLAC. This enables simulations within a single framework. Parallel implementation allows large scale computation, and high fidelity and high accuracy simulations can be performed in faster time. In this paper, TEM3P is used to analyze thermal loading in the coupler end-groups of the JLAB SCRF cavity. The results are benchmarked against measurements.

 
FR5PFP073 2D Potential for an Elliptical Charge Distribution vacuum, plasma, electromagnetic-fields 4479
 
  • K. Haghighi mood
    PPRC, Tehran
  • M. Aslaninejad
    IPM, Tehran
 
 

2D potential profiles for uniformly populated discs of charged particles with circular and elliptical cross sections inside a perfectly conducting ring are simulated using the method of images. The results are compared with the problem of infinitely long linear charge distribution inside a conducting cylinder with a dependence only on the two transverse coordinates*.


*Miguel A. Furman Phys. Rev. ST Accel. Beam 10, 081001(2007)

 
FR5PFP074 Self-Consistent Parallel Multi Bunch Beam-Beam Simulation Using a Grid-Multipole Method multipole, space-charge, interaction-region, collider 4482
 
  • F.W. Jones
    TRIUMF, Vancouver
  • W. Herr, T. Pieloni
    CERN, Geneva
 
 

The simulation code COMBI has been developed to enable the study of coherent beam-beam effects in the full collision scenario of the LHC, with multiple bunches interacting at multiple crossing points over many turns. The parallel version of COMBI was first implemented using a soft-Gaussian collision model which entails minimal communication between worker processes. Recently we have extended the code to a fully self-consistent collision model using a Grid-Multipole method, which allows worker processes to exchange charge and field information in a compact form which minimizes communication overhead. In this paper we describe the Grid-Multipole technique used and its adaptation to the parallel environment through pre- and post-processing of charge and grid data. Performance measurements in multi-core and Myrinet-cluster environments will be given. We will also present our estimates of the potential for very large-scale simulations on massively-parallel hardware, in which the number of simulated bunches ultimately approaches the actual LHC bunch population.

 
FR5PFP075 Benchmarking TRACK against PARMELA and ASTRA in the Design of the TRIUMF e-Linac cavity, linac, space-charge, electron 4485
 
  • F. Yan, Y.-C. Chao, R.E. Laxdal, M. Marchetto
    TRIUMF, Vancouver
  • S. Dechoudhury, V. Naik
    DAE/VECC, Calcutta
  • G. Goh
    SFU, Burnaby, BC
  • B. Mustapha
    ANL, Argonne
 
 

The TRIUMF ARIEL Project plans to build a 50MeV electron linac at 10mA to produce radioactive ion beams through photofission. Beam dynamics studies of the accelerator are on-going. The TRACK code originally written to simulate proton and heavy ion linacs has been used in e-linac modeling studies. This paper will summarize the TRACK simulation studies and the simulation results will be compared with other codes like PARMELA and ASTRA.

 
FR5PFP076 Multipacting Simulation in ISAC-II Superconducting Cavities cavity, multipactoring, electron, ISAC 4488
 
  • M. Gusarova, M.V. Lalayan, N.P. Sobenin
    MEPhI, Moscow
  • V. Zvyagintsev
    TRIUMF, Vancouver
 
 

The results of 3D multipacting simulation in coaxial superconducting quarter wave cavities of the linear accelerator of heavy ions ISAC-II are presented. The multipacting simulation was done using MultP-M code. Dangerous areas of structure and levels of an accelerating field are revealed. Examples of electrons resonant trajectories are presented. Simulation results are compared with experimental results obtained during several superconducting cavities processing.

 
FR5PFP078 Fringe-Field Effects in Simulations of Non-Scaling FFAGs 4492
 
  • D.T. Abell, G.I. Bell
    Tech-X, Boulder, Colorado
  • E. Forest
    KEK, Ibaraki
  • A.G. Ruggiero, D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

Funding: Supported in part by the DOE Office of Science, Office of Nuclear Physics under grant No. DE-FG02-06ER84508.


Recent simulations of non-scaling FFAGs suggest that the effects of magnet fringe fields are of signal importance. We present PTC* simulations that include realistic models for the fringes. In particular, we study how fringe extent and other parameters affect important measures of machine performance.


*E. Forest, Y. Nogiwa, F. Schmidt, "The FPP and PTC Libraries", ICAP'2006.

 
FR5PFP079 Highly Accurate Frequency Calculations of Crab Cavities Using the VORPAL Computational Framework cavity, extraction, collider, HOM 4493
 
  • T.M. Austin
    Tech-X, Boulder, Colorado
  • L. Bellantoni
    Fermilab, Batavia
  • J.R. Cary
    CIPS, Boulder, Colorado
 
 

Funding: US DOE, COMPASS SciDAC-2, Grant Number DE-FC02-07ER41499


We have applied the Werner-Cary method* for extracting modes and mode frequencies from time-domain simulations of crab cavities, as are needed for the ILC and the beam delivery system of the LHC. This method for frequency extraction relies on a small number of simulations and post-processing using the SVD algorithm with Tikhonov regularization. The time domain simulations were carried out using the VORPAL computational framework, which is based on the eminently scalable finite-difference time-domain algorithm. A validation study was performed on an aluminum model of the 3.9 GHz RF separators built originally at Fermi National Accelerator Laboratory in the US. Comparisons with measurements of the A15 cavity show that this method can provide accuracy to within 0.01% of experimental results after accounting for manufacturing imperfections. To capture the near degeneracies two simulations requiring in total a few hours on 600 processors were employed. This method has applications across many areas including obtaining MHD spectra from time-domain simulations.


*J. Comp. Phys. 227, 5200-5214 (2008)

 
FR5PFP080 Reduction of the Friction Force in Electron Cooling Systems due to Magnetic Field Errors electron, ion 4496
 
  • A.V. Sobol, G.I. Bell, D.L. Bruhwiler
    Tech-X, Boulder, Colorado
  • A.V. Fedotov, V. Litvinenko
    BNL, Upton, Long Island, New York
 
 

Funding: Supported by the US DOE Office of Nuclear Physics under grants DE-FC02-07ER41499 and DE-FG02-04ER84094; used NERSC resources under grant DE-AC02-05CH11231.


Magnetic field errors can limit the dynamical friction force on co-propagating ions and, hence, increase the cooling time. We present theoretical and numerical results for reduction of the friction force due to bounded transverse magnetic field errors, as a function of wavelength. VORPAL * simulations using a binary collision algorithm ** show that small-wavelength field errors affect the friction logarithmically, via the Coulomb log, while long-wavelength errors reduce the friction by effectively increasing the transverse electron temperature. A complete understanding of finite-time effects and the role of small impact parameter collisions is required to correctly interpret the simulation results. We show that the distribution of electron-ion impact parameters is similar to a Pareto distribution, for which the central limit theorem does not apply. A new code has been developed to calculate the cumulative distribution function of electron-ion impact parameters and thus correctly estimate the expectation value and uncertainty of the friction force.


* C. Nieter and J. Cary, J. Comp. Phys. 196 (2004), p. 448.
** G. Bell et al., J. Comp. Phys. 227 (2008), p. 8714.

 
FR5PFP081 3D Simulations of Secondary Electron Generation and Transport in a Diamond Electron Beam Amplifier electron, scattering, cathode, emittance 4497
 
  • R. Busby, J.R. Cary, D.A. Dimitrov
    Tech-X, Boulder, Colorado
  • I. Ben-Zvi, X. Chang, J.W. Keister, E.M. Muller, T. Rao, J. Smedley, Q. Wu
    BNL, Upton, Long Island, New York
 
 

Funding: The work at Tech-X Corp. is supported by the U. S. Department of Energy under the DE-FG02-06ER84509 SBIR grant.


The Relativistic Heavy Ion Collider (RHIC) contributes fundamental advances to nuclear physics by colliding a wide range of ions. A novel electron cooling section, which is a key component of the proposed luminosity upgrade for RHIC, requires the acceleration of high-charge electron bunches with low emittance and energy spread. A promising candidate for the electron source is the recently developed concept of a high quantum efficiency photoinjector with a diamond amplifier. To assist in the development of such an electron source, we have implemented algorithms within the VORPAL particle-in-cell framework for modeling secondary electron and hole generation, and for charge transport in diamond. The algorithms include elastic, phonon, and impurity scattering processes over a wide range of charge carrier energies. Results from simulations using the implemented capabilities will be presented and discussed.

 
FR5PFP082 Investigation of Charge Gain in Diamond Electron Beam Amplifiers via 3D Simulations electron, scattering, cathode, emittance 4500
 
  • D.A. Dimitrov, R. Busby, J.R. Cary
    Tech-X, Boulder, Colorado
  • I. Ben-Zvi, X. Chang, J.W. Keister, E.M. Muller, T. Rao, J. Smedley, Q. Wu
    BNL, Upton, Long Island, New York
 
 

Funding: The work at Tech-X Corp. is supported by the US DoE under grant DE-FG02-06ER84509.


A promising new concept of a diamond amplified photocathode for generation of high-current, high-brightness, and low thermal emittance electron beams was recently proposed* and is currently under active development. To better understand the different effects involved in the generation of electron beams from diamond, we have been developing models (within the VORPAL computational framework) to simulate secondary electron generation and charge transport. The currently implemented models include inelastic scattering of electrons and holes for generation of electron-hole pairs, elastic, phonon, and charge impurity scattering. We will present results from 3D VORPAL simulations with these capabilities on charge gain as a function of primary electron energy and applied electric field. Moreover, we consider effects of electron and hole cloud expansion (initiated by primary electrons) and separation in a surface domain of diamond.


*I. Ben-Zvi et al., Secondary emission enhanced photoinjector, C-AD Accel. Phys. Rep. C-A/AP/149, BNL (2004).

 
FR5PFP083 Accurate and Efficient Study of RF Cavities by Using a Conformal FDTD Method cavity 4503
 
  • M.C. Lin, C. Nieter, D.N. Smithe, P. Stoltz
    Tech-X, Boulder, Colorado
 
 

Funding: DoD FA9451-07-C-0025


This work introduces a conformal finite difference time domain (CFDTD) method as implemented in VORPAL to accurately and efficiently study RF cavities. For illustration, an A6 magnetron cavity has been employed and the corresponding dispersion relation has been carried out. The accuracy of the CFDTD method is measured by comparing with SUPERFISH calculations. To verify the accuracy of the CFDTD simulations, a geometric model has been constructed in VORPAL and simulated with different mesh numbers as 10,000, 40,000, 90,000, 160,000, and 250,000 for three DMFRAC values equal to 0.75, 0.5 and 0.25, respectively. The results show an accuracy of 99.4% can be achieved by using only 10,000 meshes with Dey-Mittra algorithm. By comparison, a mesh number of 360,000 need be used to preserve an accuracy of 99% in the conventional FDTD method. One should be careful using conventional FDTD to study systems with complicated geometry as the staircased meshes fail to conform the boundary correctly. The simulation time of studying the interaction of particles with fields inside cavities can be dramatically reduced by using CFDTD particle-in-cell simulation without losing accuracy.


* C. Nieter, J. R. Cary, J. Comput. Phys. 196, 448-473 (2004).
** S. Dey, R. Mittra, and S. Chebolu, Microwave and Opt. Technol. Lett. 14, 213-215 (1997).

 
FR5PFP084 Fast Electromagnetic Solver for Cavity Optimization Problems cavity, plasma, electromagnetic-fields 4504
 
  • P. Messmer, T.M. Austin, J.R. Cary
    Tech-X, Boulder, Colorado
 
 

Funding: This project was in part supported by DOE Office of Advanced Scientific Computing Research SBIR Phase II grant #DE-FG02-07ER84731, SciDAC Grant #DE-FC02-07ER41499, and Tech-X Corporation.


In order to meet the design and budget constraints of next generation particle accelerators, individual components have to be optimized using numerical simulations. Among the optimizations are the geometric shape of RF cavities and the placement of coupler and dampers, requiring large numbers of simulations. It is therefore desirable to accelerate individual cavity simulations. Finite-Difference Time-Domain (FDTD) is a widely used algorithm for modeling electromagnetic fields. While being a time-domain algorithm, it can also be used to determine cavity modes and their frequencies. Weak scaling of parallel FDTD yields good results due to the algorithm locality, but the maximum speedup is determined by the usually small problem size. Graphics Processing Units (GPUs) offer a huge amount of processing power and memory bandwidth, well suited for accelerating FDTD simulations. We therefore developed an FDTD solver on GPUs and incorporated it into the plasma simulation code VORPAL. We will present GPU accelerated VORPAL simulations, provide speedup figures and address the effect of running these simulations in single precision.

 
FR5PFP085 Benchmarking Multipacting Simulations in VORPAL electron, cavity, resonance, plasma 4505
 
  • C. Nieter, C. Roark, P. Stoltz
    Tech-X, Boulder, Colorado
  • K. Tian
    JLAB, Newport News, Virginia
 
 

Funding: Department of Energy SBIR grant DE-FG02-05ER84172


We will present the results of benchmarking simulations run to test the ability of VORPAL to model multipacting processes in Superconducting Radio Frequency structures. VORPAL is an electromagnetic (FDTD) particle-in-cell simulation code originally developed for applications in plasma and beam physics. The addition of conformal boundaries and algorithms for secondary electron emission allow VORPAL to be applied to multipacting processes. We start with simulations of multipacting between parallel plates where there are well understood theoretical predictions for the frequency bands where multipacting is expected to occur. We reproduce the predicted multipacting bands and demonstrate departures from the theoretical predictions when a more sophisticated model of secondary emission is used. Simulations of existing cavity structures developed at Jefferson National Laboratories will also be presented where we compare results from VORPAL to experimental data.

 
FR5PFP086 HOM Maps of RF Cavities for Particle Tracking Codes cavity, HOM 4508
 
  • I.V. Pogorelov, D.T. Abell, P. Stoltz
    Tech-X, Boulder, Colorado
 
 

Funding: Supported in part by the DOE Office of Science, Office of High-Energy Physics under grant No. DE-FG02-06ER84485.


We present our recently developed capability for generating High-Order Mode (HOM) maps of rf cavity fields for use in particle tracking code-based simulations. We use VORPAL field data as a starting point, and follow the approach of* to produce the maps that are subsequently incorporated into the MaryLie/IMPACT and Synergia frameworks. We present and discuss the results of applying this new modeling tool to crab cavity simulations.


*D.T. Abell, "Numerical computation of high-order transfer maps for rf cavities", Phys. Rev. ST Accel. Beams 9, 052001, (2006).

 
FR5PFP088 New Diffusion Analysis Tools for Beam Beam Simulations dynamic-aperture, emittance, extraction, site 4509
 
  • V.H. Ranjbar, A.V. Sobol
    Tech-X, Boulder, Colorado
  • H.J. Kim, T. Sen
    Fermilab, Batavia
 
 

Funding: This work was supported by the US DOE Office of Science, Office of Nuclear Physics, under Grant No. DE-FG02-08ER85183


A new set of tools for BBSIM has recently been developed to analyze the nature of the diffusion in multi-particle simulations. The diffusion subroutines are currently used to accelerate beam lifetime calculations by estimating the diffusion coefficient at various actions and integrating the diffusion equation. However it is possible that there may be regimes where anomalous diffusion dominates and normal diffusion estimates are incorrect. The tools we have developed estimate the deviation from normal diffusion and can fit the coefficients of a jump diffusion model in the event that this type of diffusion dominates.

 
FR5PFP089 Modeling Microwave Transmission in Electron Clouds electron, resonance, plasma, dipole 4512
 
  • S.A. Veitzer, P. Stoltz
    Tech-X, Boulder, Colorado
  • J.M. Byrd
    LBNL, Berkeley, California
  • K.G. Sonnad
    FZK, Karlsruhe
 
 

Funding: This work funded by the Department of Energy under Small Business Innovation Research Contract No. DE-FG02-08ER85042.


Microwave transmission in accelerator beam pipes is providing a unique method for determining electron cloud characteristics, such as density, plasma temperature, and potentially the efficacy of electron cloud mitigation techniques. Physically-based numerical modeling is currently providing a way to interpret the experimental data, and understand the plasma-induced effects on rf signals. We report here recent applications of numerical simulation of microwave transmission in the presence of electron clouds. We examine the differences in phase shift induced by TE11 and TM01 modes in circular cross section beam pipes for uniform density electron clouds. We also detail numerical simulation of the cyclotron resonance and examine how the width of the resonance changes with applied dipole magnetic fields strength and cloud temperature.

 
FR5PFP090 Handling Overlapping Fields within the V-Code Beam Dynamics Simulation Tool quadrupole, dipole, focusing, electron 4513
 
  • S. Franke, W. Ackermann, T. Weiland
    TEMF, TU Darmstadt, Darmstadt
  • J. Enders, C. Heßler, Y. Poltoratska
    TU Darmstadt, Darmstadt
 
 

Funding: This work was supported by DFG through SFB 634.


Based on the moment approach a fast tracking code named V-Code has been implemented at TEMF. Instead of using the particle distribution itself this method applies a discrete set of moments of the particle distribution. The time evolution of each moment can be deduced from the Vlasov equation when all essential external forces are known. These forces are given by the Lorentz equation in combination with the distribution of electric and magnetic fields. For efficiency reasons the 3D fields in the vicinity of the bunch trajectory are reconstructed in V-Code from one-dimensional field components by means of proper multipole expansions for the individual beam line elements. The entire beam line is represented in the code as a successive alignment of separate independent beam line elements. The proximity of some beam forming elements may lead to overlapping fringe fields between consecutive elements. In order to simulate even such beam lines with the V-Code, its database of disjunctive beam line elements has to be enhanced to deal also with superposed fields. In this paper a summary of issues regarding the implementation complemented with simulation results will be provided.

 
FR5PFP091 Wakefield Computations with the PBCI Code Using a Non-Split Finite Volume Method controls, wakefield, cavity, HOM 4516
 
  • E. Gjonaj, T. Lau, T. Weiland
    TEMF, TU Darmstadt, Darmstadt
 
 

We report on a new numerical technique for the computation of geometrical wakes in three-dimensional LINAC structures. The method utilises an explicit Finite-Volume Time-Domain (FVTD) formulation. The numerical dispersion in all three axial directions is completely eliminated by choice of an appropriate staggering of the field components on the grid. Thus, contrary to most of the previously reported techniques no splitting of the time-evolution operator is necessary. This results in large savings in computational time as well as in an improved numerical accuracy. We have implemented this new technique in PBCI code and present some preliminary results.

 
FR5PFP096 Updates to QUINDI – A Code to Simulate Coherent Emission from Bending Systems radiation, electron, acceleration, quadrupole 4526
 
  • D. Schiller
    UCLA, Los Angeles, California
  • S. Reiche
    PSI, Villigen
 
 

QUINDI has been developed to address the numerical challenge of calculating the radiation spectra from electron bunches in bending magnet systems. Since the introduction of QUINDI, many improvements and features have been added. QUINDI now supports a 3D model for bending magnets which includes fringing fields. A more modular approach has been achieved which allows better interoperability with other tracking and radiation codes. There have been many updates to the electric field calculation and spectrum processing, as well as to the post-processor, SpecGUI.

 
FR5PFP097 Implementation of Coupler RF Kick & Coupler Wake Field Effects in Lucretia emittance, linac, wakefield, cavity 4529
 
  • A. Saini
    University of Delhi, Delhi
  • A. Latina, J.-F. Ostiguy, K. Ranjan, N. Solyak, V.P. Yakovlev
    Fermilab, Batavia
 
 

It is well known that Insertion of a coupler into a RF cavity breaks the rotational symmetry of the cavity, resulting in an asymmetric field. This asymmetric field results in a transverse RF Kick*. This RF kick transversely offsets the bunch from the nominal axis & it depends on the longitudinal position of the particle in the bunch. Also, insertion of coupler generates short range transverse wake field** which is independent from the transverse offset of the particle. These effects cause emittance dilution and it is thus important to study their behavior & possible correction mechanisms. These coupler effects, i.e. coupler’s RF kick & coupler's wake field are implemented in a beam dynamics program, Lucretia. Calculations are done for Main Linac. For ILC like Lattices Results are compared with analytical results. and a good agreement has been found.


*N.Solyak et al, “RF Kick in the ILC Acceleration Structure. ” MOPP042.pdf (EPAC 08).
** N.Solyak et al, “Transverse Wake Field Simulation for the ILC Acceleration Structure”. MOPP043 pdf (EPAC 08).

 
FR5PFP098 Self-Consistent Non-Stationary Model for Multipactor Analysis in Dielectric-Loaded Accelerator Structures electron, multipactoring, vacuum, space-charge 4532
 
  • O.V. Sinitsyn, T.M. Antonsen, R.A. Kishek, G.S. Nusinovich
    UMD, College Park, Maryland
 
 

Funding: Office of High Energy Physics, US Department of Energy (DoE).


Multipactor (MP) may occur in many situations: one- and two-surface MP, resonant and poly-phase-MP, on the surface of metals and dielectrics etc. We consider this phenomenon in dielectric loaded accelerator (DLA) structures. The starting point for our work is experimental and theoretical studies of such structures jointly done by Argonne National Lab and Naval Research Lab*. In the theoretical model developed during those studies, the space charge field due to the accumulated charged particles is taken into account as a parameter. We offer a non-stationary 2D cylindrical model where the DC field is taken into account self-consistently. We have improved our previous model** and demonstrated that its predictions are in good agreement with the results of other studies***. We also demonstrate some recent results where the effects of axial particle motion are taken into account.


*J.G. Power et al., PRL, 92, 164801, 2004
**O.V. Sinitsyn et. al., AIP Proc. 13th Advanced Accelerator Concepts, 2008
***J.G. Power, S.H. Gold, AIP Proc.12th Advanced Accelerator Concepts, 2006

 
FR5RFP003 Optimization of a Truncated Photonic Crystal Cavity for Particle Acceleration cavity, lattice, higher-order-mode, acceleration 4541
 
  • C.A. Bauer, J.R. Cary, G.R. Werner
    CIPS, Boulder, Colorado
 
 

Funding: This work is supported by the U.S. Department of Energy grant DE-FG02-04ER41317.


Through computer simulation, a 2D photonic crystal (PhC) cavity formed from a truncated triangular lattice of dielectric rods is optimized to confine a single accelerating mode efficiently. Photonic crystals have the ability to reflect radiation within only certain frequency ranges, called bandgaps; the bandgaps are determined by the geometry and material of the PhC and so are tunable. For truncated PhCs, reflection is incomplete. Therefore, the confinement of bandgap frequencies to a cavity within a truncated PhC is weakened by the severity of the truncation. For a cavity made of 18 dielectric rods in a truncated triangular lattice arrangement, the desired accelerating cavity mode is weakly confined. Adjusting the positions and sizes of the dielectric rods away from the best lattice configuration within an optimization procedure gives unintuitive structures, ultimately increasing the confinement of the accelerating mode by a factor of 100. Confinement of higher-order modes is also dramatically reduced by the optimization. Similar increases in confinement of the fundamental accelerating mode are found for a 24-rod structure.

 
FR5RFP007 Capture and Control of Laser-Accelerated Proton Beams: Experiment and Simulation proton, solenoid, laser, target 4545
 
  • F. Nürnberg, B.G. Logan
    LBNL, Berkeley, California
  • I. Alber, K. Harres, M. Roth, M. Schollmeier
    TU Darmstadt, Darmstadt
  • W.A. Barth, H. Eickhoff, I. Hofmann
    GSI, Darmstadt
  • A. Friedman, D.P. Grote
    LLNL, Livermore, California
 
 

Ion acceleration from high-intensity, short-pulse laser irradiated thin foils has attracted much attention during the past decade. The emitted ion and, in particular, proton pulses contain large particle numbers (exceeding a trillion particles) with energies in the multi-MeV range and are tightly confined in time (< ps) and space (source radius a few micrometers). The generation of these high-current beams is a promising new area of research and has motivated pursuit of applications such as tabletop proton sources or pre-accelerators. Requirements for an injector are controllability, reproducibility and a narrow (quasi-monoenergetic) energy. However, the source provides a divergent beam with an exponential energy spectrum that exhibits a sharp cutoff at its maximum energy. The laser and plasma physics group of the TU Darmstadt, in collaboration with GSI and LBNL, is studying possibilities for transport and RF capture in conventional accelerator structures. First results on controlling laser-accelerated proton beams are presented, supported by WARP simulations.

 
FR5RFP012 Epicyclic Helical Channels for Parametric Resonance Ionization Cooling resonance, solenoid, beam-transport, luminosity 4554
 
  • A. Afanasev, K.B. Beard, V. Ivanov, R.P. Johnson, G.M. Wang
    Muons, Inc, Batavia
  • A. Afanasev
    Hampton University, Hampton, Virginia
  • S.A. Bogacz, Y.S. Derbenev
    JLAB, Newport News, Virginia
  • K. Yonehara
    Fermilab, Batavia
 
 

Funding: Work supported in part in part by DOE contract DE-AC02-07CH11359 and DOE STTR Grant DE-FG02-05ER86253


In order to achieve cooling of muons in addition to 6D helical cooling channel (HCC) [1], we develop a technique based on a parametric resonance. The use of parametric resonances requires alternating dispersion, minimized at locations of thin absorbers, but maximized in between in order to compensate for chromatic aberrations [2]. These solutions can be combined in an Epicyclic Helical Cooling Channel (EHCC) that meets requirements of alternating dispersion of beam periodic orbit with best conditions for maintenance of stable beam transport in a continuous solenoid-type field [3]. We discuss here basic features and new simulation results for EHCC.

 
FR5RFP014 Testing of Laser-Driven Resonant Accelerating-Structures Possessing Sub-Wavelength Periodic Features laser, alignment, resonance, controls 4559
 
  • N. Vartanian, G. Travish
    UCLA, Los Angeles
  • E.R. Arab
    PBPL, Los Angeles
 
 

The Micro-Accelerator Platform, a laser-driven accelerating device measuring less than a millimeter in each dimension, has a variety of applications in industry and medicine. The structure consists of two parallel slabs, with each possessing reflective surfaces and with one having periodic slots which allows transversely incident laser light to enter the gap between the two planes. The resonance of the electric field created in the gap can be measured indirectly through the spectral response of the device. Using a combination of an interferometer and a fiber coupled spectrometer, prototype structures are aligned and measured. With the aid of a nanometer-accuracy positioning device, the bottom slab (a mirror) is aligned with the top slotted-structure. The interferometer and a low power laser are used to position the slabs. A 800nm Titanium-Sapphire oscillator with a bandwidth of greater than 100nm is used for the spectral measurements. The spectra of both transmitted and reflected beams have been measured for a number of structures and are compared to simulation results. Various improvements to the initial measurement system as well as alternative future approaches are discussed.

 
FR5RFP015 Testing of a Laser-Powered, Slab-Symmetric Dielectric Structure for Medical and Industrial Applications laser, electron, coupling, radiation 4562
 
  • S. Boucher, P. Frigola
    RadiaBeam, Marina del Rey
  • E.R. Arab, G. Travish, N. Vartanian
    UCLA, Los Angeles, California
  • R.B. Yoder
    Manhattanville College, Purchase, NY
 
 

Funding: This project is supported by DOE SBIR Grant DE-FG02-08ER85038.


Laser-powered dielectric accelerating structures, which have attracted attention in recent years, trade fabrication challenges and extremely small beam apertures for the promise of high gradients and new bunch formats. The slab-symmetric, periodically-coupledμAccelerator Platform (MAP) is one such dielectric accelerator, and has been under development through a RadiaBeam-UCLA collaboration for several years. Intended applications of the structure include the production of radiation for medical treatments, imaging, and industrial uses. Prototype MAP structures are now being fabricated, and a program has been undertaken to test this device using externally injected electron beams. Plans are underway to install structures in the E163 facility at SLAC. In this paper we describe the testing methods, diagnostics and expectations. Progress and results to date are also presented.

 
FR5RFP016 Scaling and Transformer Ratio in a Plasma Wakefield Accelerator wakefield, plasma, electron, acceleration 4565
 
  • I. Blumenfeld, F.-J. Decker, M.J. Hogan, R. Ischebeck, R.H. Iverson, N.A. Kirby, R. Siemann, D.R. Walz
    SLAC, Menlo Park, California
  • C.E. Clayton, C. Huang, C. Joshi, W. Lu, K.A. Marsh, W.B. Mori, M. Zhou
    UCLA, Los Angeles, California
  • T.C. Katsouleas, P. Muggli, E. Oz
    USC, Los Angeles, California
 
 

High gradient acceleration of electrons has recently been achieved in meter scale plasmas at SLAC. Results from these experiments show that the wakefield is sensitive to parameters in the electron beam which drives it. In the experiment the bunch lengths were varied systematically at constant charge. Here we investigate the correlation of peak beam current to the wake amplitude. The effect of beam head erosion will be discussed and an experimental limit on the transformer ratio set. The results are compared to simulation.

 
FR5RFP017 Investigation of a Gas Jet-Produced Hollow Plasma Wakefield Accelerator plasma, ion, electron, positron 4566
 
  • N.A. Kirby, I. Blumenfeld, M.J. Hogan, R. Siemann, D.R. Walz
    SLAC, Menlo Park, California
  • A.W. Davidson, C. Huang
    UCLA, Los Angeles, California
 
 

The effect of ion motion and the need for practical positron propagation in a plasma wakefield accelerator (PWFA) have incited interest in hollow plasma channels. These channels are typically assumed to be cylindrically symmetric; however, a different geometry might be easier to achieve. The introduction of an obstruction into the outlet of a high Mach number gas jet can produce two parallel slabs of gas separated by a density depression. Here, there is a detailed simulation study of the density depression created in such a system. This investigation reveals that the density depression is insufficient at the desired plasma density. However, insights from the simulations suggest another avenue for the creation of the hollow slab geometry.

 
FR5RFP018 Laser Wakefield Simulation Using a Speed-of-Light Frame Envelope Model laser, wakefield, injection, plasma 4569
 
  • B.M. Cowan, D.L. Bruhwiler, P. Messmer, K. Paul
    Tech-X, Boulder, Colorado
  • E. Cormier-Michel, E. Esarey, C.G.R. Geddes
    LBNL, Berkeley, California
 
 

Funding: Work supported by Department of Energy contracts DE-AC02-05CH11231 (LBNL), DE-FC02-07ER41499 (SciDAC), and DE-FG02-04ER84097 (SBIR).


Simulation of laser wakefield accelerator (LWFA) experiments is computationally highly intensive due to the disparate length scales involved. Current experiments extend hundreds of laser wavelengths transversely and many thousands in the propagation direction, making explicit PIC simulations enormously expensive. We can substantially improve the performance of LWFA simulations by modeling the envelope modulation of the laser field rather than the field itself. This allows for much coarser grids, since we need only resolve the plasma wavelength and not the laser wavelength, and this also allows larger timesteps. Thus an envelope model can result in savings of several orders of magnitude in computational resources. By propagating the laser envelope in a Galilean frame moving at the speed of light, dispersive errors can be avoided and simulations over long distances become possible. Here we describe the model and its implementation. We show rigorous studies of convergence and discretization error, as well as benchmarks against explicit PIC. We also demonstrate efficient, fully 3D simulations of downramp injection and meter-scale acceleration stages.

 
FR5RFP025 Simulations of Positron Beams Propagating in Plasma plasma, emittance, positron, focusing 4586
 
  • X. Li, P. Muggli
    USC, Los Angeles, California
  • S.F. Martins
    UCLA, Los Angeles, California
 
 

Funding: Work supported by the US Department of Energy


Studies on propagation of electron beams in plasma have shown that in the blowout regime of the plasma wakefield accelerator (PWFA), the emittance of the incoming beam is preserved because of the linear focusing force exerted by a uniform ion column [1]. However, for positron beams the focusing force is nonlinear and they suffer emittance growth. We simulated the propagation of a positron beam in the uniform plasmas with different densities. We calculated the beam emittance from the simulation results and observed the beam size and emittance grow with increasing plasma density. Simulation results agree well with that of previous work.

 
FR5RFP030 Landau Damping with High Frequency Impedance impedance, synchrotron, damping, cavity 4592
 
  • M. Blaskiewicz
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under contract No. DE-AC02-98CH10886 with the U.S. Department of Energy


Couples bunch longitudinal instability in the presence of high frequency impedance is considered. A frequency domain technique is developed and compared with simulations. The frequency domain technique allows for absolute stability tests and is applied to the problem of longitudinal stability in RHIC with the proposed 56 MHz rf system.

 
FR5RFP033 Microwave Instability Simulations for NSLS-II vacuum, cavity, undulator, damping 4601
 
  • A. Blednykh, S. Krinsky, B. Nash, L.-H. Yu
    BNL, Upton, Long Island, New York
 
 

For the NSLS-II storage ring with damping wigglers but without a Landau cavity, the low-current bunch length is 4.5mm. We have studied bunch lengthening and estimated the microwave instability threshold using the multi-particle tracking code TRANFT. An estimate of the pseudo-Green’s function for a 0.5mm driving bunch was obtained for most components of the vacuum system by using the 3D code GdfidL. With our present computer resources, certain components were too large and had too complex geometry to allow the wake for such a short bunch to be computed using GdFidL. In these cases, the actual 3D geometry was approximated by a structure having circular cross-section, and the pseudo-Green’s function was computed using the 2D code ABCI. It was found that the dominant geometric wake is due to the tapers for the in-vacuum undulators. The resistive wall wake is also important. The effect of pseudo-Green’s functions corresponding to an even shorter driving bunch (0.05mm) was investigated using the program ECHO to compute the wake of tapers with circular cross-section. Our results suggest that the microwave threshold will occur at an average single-bunch current greater than 5mA.

 
FR5RFP040 Wake Field Simulations for the Vacuum Chamber Transitions of the ILC Damping Ring wakefield, impedance, damping, vacuum 4619
 
  • M. Korostelev, A. Wolski
    Cockcroft Institute, Warrington, Cheshire
  • N.A. Collomb, J.M. Lucas
    STFC/DL, Daresbury, Warrington, Cheshire
  • O.B. Malyshev
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

Vacuum chamber transitions of the ILC damping rings associated with BPM insertions, vacuum ports, antechamber tapers etc, may make a significant contribution to the overall machine impedance. Since most transitions are not azimuthally symmetric, commercial 3D codes based on the finite element method have been used to compute their wake fields. The results for selected vacuum chamber components are presented in this paper, together with some estimates of the impact of the wake fields on the beam dynamics in the damping rings.

 
FR5RFP041 Full Structure Simulations of ILC Collimators wakefield, vacuum, linear-collider, collider 4622
 
  • J.D.A. Smith
    Cockcroft Institute, Warrington, Cheshire
 
 

The prototype collimator of the ILC is simulated, to address potential issues with trapped modes and heating. A number of codes are benchmarked, and the interplay between resistive and geometric wakefields is carefully considered.

 
FR5RFP043 Simulations of Electron-Cloud Current Density Measurements in Dipoles, Drifts and Wigglers at CesrTA wiggler, electron, dipole, positron 4628
 
  • J.R. Calvey, J.A. Crittenden, G. Dugan, S. Greenwald, D.L. Kreinick, J.A. Livezey, M.A. Palmer, D. L. Rubin
    CLASSE, Ithaca, New York
  • C.M. Celata, M.A. Furman, G. Penn, M. Venturini
    LBNL, Berkeley, California
  • K.C. Harkay
    ANL, Argonne
  • P. Jain, K. Kanazawa, Y. Suetsugu
    KEK, Ibaraki
  • M.T.F. Pivi, L. Wang
    SLAC, Menlo Park, California
 
 

Funding: Supported by the US National Science Foundation, the US Department of Energy under Contracts No. DE-AC02-06CH11357, DE-AC02-05CH11231, and DE-AC02-76SF00515, and by the Japan/US Cooperation Program.


CESR at Cornell has been operating as a damping ring test accelerator (CesrTA) with beam parameters approaching those anticipated for the ILC damping rings. A core component of the research program is to fully understand electron cloud effects in CesrTA. As a local probe of the electron cloud, several segmented retarding field analyzers (RFAs) have been installed in CesrTA in dipole, drift and wiggler regions. Using these RFAs, the energy spectrum of the time-average electron cloud current density striking the walls has been measured for a variety of bunch train patterns; with bunch populations up to 2x1010 per bunch, beam energies from 2 to 5 GeV, horizontal geometric emittances from roughly 10 to 133 nm, and bunch lengths of about 1 cm; and for both positron and electron beams. The effect of mitigation measures, such as coatings, has also been studied. This paper will compare these measurements with the predictions of simulation programs, and discuss the implications of these comparisons for our understanding of the physics of electron cloud generation and mitigation in ILC-like damping rings.

 
FR5RFP044 Studies of the Effects of Electron Cloud Formation on Beam Dynamics at CesrTA electron, dipole, positron, photon 4631
 
  • J.A. Crittenden, J.R. Calvey, G. Dugan, D.L. Kreinick, J.A. Livezey, M.A. Palmer, D. L. Rubin
    CLASSE, Ithaca, New York
  • M.A. Furman, G. Penn, M. Venturini
    LBNL, Berkeley, California
  • K.C. Harkay
    ANL, Argonne
  • R. Holtzapple
    CalPoly, San Luis Obispo, CA
  • K. Ohmi
    KEK, Ibaraki
  • M.T.F. Pivi, L. Wang
    SLAC, Menlo Park, California
 
 

Funding: National Science Foundation award 0734867 Office of Science, U.S. Department of Energy contracts DE-AC02-05CH11231 and DE-AC02-06CH11357


The Cornell Electron Storage Ring Test Accelerator (CesrTA) has commenced operation as a linear collider damping ring test bed following its conversion from an e+e- collider in 2008. A core component of the research program is the measurement of effects of synchrotron-radiation-induced electron cloud formation on beam dynamics. We have studied the interaction of the beam with the cloud in a number of experiments, including measurements of coherent tune shifts and emittance growth in various bunch train configurations, with different bunch currents, beam energies, beam emittance, and bunch lengths, for both positron and electron beams. This paper compares these measurements to modeling results from several advanced cloud simulation algorithms and discusses the implications of these comparisons for our understanding of the physics of electron cloud formation and decay in damping rings of the type proposed for future high-energy linear colliders.

 
FR5RFP047 Analysis of the Transverse SPS Beam Coupling Impedance with Short and Long Bunches impedance, kicker, pick-up, resonance 4640
 
  • B. Salvant
    EPFL, Lausanne
  • G. Arduini, H. Burkhardt, H. Damerau, W. Höfle, E. Métral, G. Papotti, G. Rumolo, B. Salvant, R. Tomás, S.M. White
    CERN, Geneva
  • R. Calaga, R. De Maria
    BNL, Upton, Long Island, New York
 
 

The upgrade of the CERN Large Hadron Collider (LHC) would require a four- to fivefold increase of the single bunch intensity presently obtained in the Super Proton Synchrotron (SPS). Operating at such high single bunch intensities requires a detailed knowledge of the sources of SPS beam coupling impedance, so that longitudinal and transverse impedance reduction campaigns can be planned and performed effectively if needed. In this paper, the transverse impedance of the SPS is studied by injecting a single long bunch into the SPS, and observing its decay without RF. This particular setup enhances the resolution of the frequency analysis of the longitudinal and transverse bunch signals acquired with strip line couplers connected to a fast data acquisition. It also gives access to the frequency content of the transverse impedance. Results from measurements with short and long bunches in the SPS performed in 2008 are compared with simulations and theoretical predictions.

 
FR5RFP048 An Update of ZBASE, the CERN Impedance Database impedance, kicker, coupling, space-charge 4643
 
  • B. Salvant
    EPFL, Lausanne
  • H. Medina, E. Métral, G. Rumolo, B. Salvant
    CERN, Geneva
 
 

A detailed knowledge of the beam coupling impedance of the CERN synchrotrons is required in order to identify the impact on instability thresholds of potential changes of beam parameters, as well as additions, removal or modifications of hardware. To this end, an update of the impedance database was performed, so that impedance results from theoretical calculations using new multilayer models, impedance results from electromagnetic field simulations and impedance results from bench measurements can be compiled. In particular, the impedance database is now set to separately produce the dipolar and quadrupolar transverse impedance and wakes that the HEADTAIL simulation code needs to accurately simulate the effect of the impedance on the beam dynamics.

 
FR5RFP049 Coupling Impedance of the CERN SPS Beam Position Monitors impedance, resonance, coupling, cavity 4646
 
  • B. Salvant
    EPFL, Lausanne
  • D. Alesini, M. Migliorati, B. Spataro
    INFN/LNF, Frascati (Roma)
  • G. Arduini, C. Boccard, F. Caspers, A. Grudiev, O.R. Jones, E. Métral, G. Rumolo, B. Salvant, C. Zannini
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
  • F. Roncarolo
    UMAN, Manchester
 
 

A detailed knowledge of the beam coupling impedance of the CERN Super Proton Synchrotron (SPS) is required in order to operate this machine with a higher intensity for the foreseen Large Hadron Collider (LHC) luminosity upgrade. A large number of Beam Position Monitors (BPM) is currently installed in the SPS, and this is why their contribution to the SPS impedance has to be assessed. This paper focuses on electromagnetic simulations and bench measurements of the longitudinal and transverse impedance generated by the horizontal and vertical BPMs installed in the SPS machine.

 
FR5RFP050 Beam Instabilities Studies at Transition Crossing in the CERN Proton Synchrotron space-charge, impedance, proton, collective-effects 4649
 
  • S. Aumon, W. Bartmann, S.S. Gilardoni, E. Métral, G. Rumolo, R.R. Steerenberg
    CERN, Geneva
  • B. Salvant
    EPFL, Lausanne
 
 

The CERN PS crosses transition energy at about 6 GeV by using a second order gamma jump performed with special quadrupoles. However, for high-intensity beams, and in particular the single bunch beam for the neutron Time-of-Flight facility, a controlled longitudinal emittance blow-up is still needed to prevent a fast single-bunch vertical instability from developing near transition. A series of studies have been done in the PS in 2008 to measure the beam behaviour near transition energy for different settings of the gamma transition jump. The purpose of this paper is to compare those measurements with simulations results from the HEADTAIL code, which should allow to understand better the different mechanisms involved and maybe improve the transition crossing.

 
FR5RFP054 Multi-Bunch Simulations with HEADTAIL impedance, wakefield, single-bunch, synchrotron 4661
 
  • G. Rumolo, E. Métral
    CERN, Geneva
 
 

The HEADTAIL code has been used for many years to study the interaction of a single bunch with a localized or lumped source of electromagnetic perturbation, usually self-induced (impedance, electron cloud or space charge). It models the bunch as macroparticles and at each turn slices up the bunch into several adjacent charged disks, which are made to subsequently interact with the perturbing agent. A first step toward the extension of HEADTAIL to multi-bunch simulations is presented in this paper. In this case, the bunches themselves are modeled as charged disks and are not sliced, which makes us lose information on the intra-bunch motion but can describe a zero mode interaction between different bunches in a train. The interaction of an SPS bunch train of 72 bunches with the resistive wall or a narrow-band impedance is studied as an example.

 
FR5RFP056 Reference Measurements of the Longitudinal Impedance in the CERN SPS impedance, quadrupole, emittance, kicker 4667
 
  • E.N. Shaposhnikova, T. Bohl, H. Damerau, K. Hanke, T.P.R. Linnecar, B. Mikulec, J. Tan, J. Tuckmantel
    CERN, Geneva
 
 

First reference measurements of the longitudinal impedance were made with beam in the SPS machine in 1999 to quantify the results of the impedance reduction programme, completed in 2001. The 2001 data showed that the low-frequency inductive impedance had been reduced by a factor 2.5 and that bunch lengthening due to the microwave instability was absent up to the ultimate LHC bunch intensity. Measurements of the quadrupole frequency shift with intensity in the following years suggest a significant increase in impedance (which nevertheless remains below the 1999 level) due to the installation of eight extraction kickers for beam transfer to the LHC. Microwave instability is still not observed up to the maximum bunch intensities available from injector. The experimental results are compared with expectations based on the known longitudinal impedance of the different machine elements in the SPS.

 
FR5RFP058 Stabilizing Effect of a Double-Harmonic RF System in the CERN PS synchrotron, emittance, impedance, cavity 4670
 
  • C.M. Bhat
    Fermilab, Batavia
  • F. Caspers, H. Damerau, S. Hancock, E. Mahner, F. Zimmermann
    CERN, Geneva
 
 

Funding: Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the U.S. Department of Energy and CARE-HHH


Motivated by the discussions on scenarios for LHC upgrades, beam studies on the stability of flat bunches in a double-harmonic RF system have been conducted in the CERN Proton Synchrotron (PS). Injecting nearly nominal LHC beam intensity per cycle, 18 bunches are accelerated on harmonic h=21 to 26 GeV with the 10 MHz RF system. On the flat-top, all bunches are then transformed to flat bunches by adiabatically adding RF voltage at h=42 from a 20 MHz cavity in anti-phase to the h=21 system. The voltage ratio V(h42)/V(h21) of about 0.5 was set according to simulations. For the next 140 ms, longitudinal profiles show stable bunches in the double harmonic RF bucket until extraction. Without the second harmonic component, coupled-bunch oscillations are observed. The flatness of the bunches along the batch is analyzed as a measure of the relative phase error between the RF systems due to beam loading. Measurements of electron cloud effects induced by the beam are also discussed. The results of beam dynamics simulations and their comparison with the measured data are presented.

 
FR5RFP066 Higher Order Modes in a String of Multi-Cell Accelerating Structures higher-order-mode, damping, linac, linear-collider 4685
 
  • Y. Morozumi
    KEK, Ibaraki
 
 

The International Linear Collider will employ tens of thousands of superconducting 9-cell accelerating structures for its main linacs. Damping of higher order modes is crucial to beam stability. Study of higher order modes, however, tends to focus on trapped modes in a single 9-cell structure model alone both in simulation and measurement. Propagating modes above cut-off frequencies are left untouched because of difficulty of a realistic model of multiple 9-cell structures. We have simulated a full spectrum of higher order modes in a long string of 9-cell structures.

 
FR5RFP067 Fast Head Tail Instability due to Electron Cloud under the Presence of the Dispersion electron, wakefield, damping, synchrotron 4686
 
  • K. Ohmi
    KEK, Ibaraki
  • J. Hyunchang
    POSTECH, Pohang, Kyungbuk
 
 

Electron cloud causes a transverse single bunch instability above a threshold of the cloud density. The threshold is determeined by the strength of the beam-electron cloud interaction and Landau damping due to the synchrotron oscillation and/or momentum compaction. We discuss that the threshold is remarkably degraded due to the dispersion, one of the parameter of the circular accelerator optics. The single bunch instability is more serious than previous predictions without considering the dispersion, especially in the case that the horizontal beam size due to the dispersion dominates compare than that due to the emittance.

 
FR5RFP070 A Simulation Study of the Electron Cloud Instability at DAΦNE electron, positron, wiggler, space-charge 4695
 
  • T. Demma, A. Drago, S. Guiducci, M. Zobov
    INFN/LNF, Frascati (Roma)
  • K. Ohmi
    KEK, Ibaraki
 
 

Funding: Work supported in part by the “Ministero degli Affari Esteri, Direzione Generale per la Promozione e la Cooperazione Culturale”


A strong horizontal instability has been observed in the DAΦNE positron ring since 2003. Experimental observations suggest an electron cloud induced coupled bunch instability as a possible explanation. In this communication we present a simulation study of the electron cloud coupled bunch instability for the DAΦNE positron ring, performed with the code PEI-M, and compare the numerical results with experimental observations.

 
FR5RFP071 Maps for Electron Clouds: Application to LHC Conditioning electron, vacuum, dipole, proton 4698
 
  • T. Demma, R. Cimino, A. Drago
    INFN/LNF, Frascati (Roma)
  • S. Petracca
    U. Sannio, Benevento
  • A. Stabile
    INFN-Salerno, Baronissi, Salerno
 
 

The electron cloud driven effects can limit the ability of recently build or planned accelerators to reach their design parameters. The secondary emission yield reduction (called "scrubbing") due to the fact that the electrons of the cloud hit the vacuum chamber wall, modifying its surface properties, may minimize any disturbing effects of the cloud to the beam. The dependence of "scrubbing" efficiency on beam and chamber parameters can be deduced from e-cloud simulation codes modeling the involved physics in full detail. In this communication we present a generalization of the map formalism, introduced in*,**, for the analysis of electron flux at the chamber wall with particular reference to the exploration of LHC conditioning scenarios. Simulations based on this formalism are orders of magnitude faster compared to those based on standard particle tracking codes.


*U.Iriso and S.Peggs, ”Maps for Electron Clouds”, Phys. Rev. ST-AB 8, 024403, 2005.
**T.Demma et al., ”Maps for Electron Clouds: Application To LHC”, Phys. Rev. ST-AB 10, 114401 (2007).

 
FR5RFP072 Stabilization of Beam Instability due to Space-Charge Effects at J-PARC space-charge, kicker, impedance, injection 4701
 
  • Y. Shobuda
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  • Y.H. Chin, M. Ikegami, T. Toyama
    KEK, Ibaraki
 
 

Kicker magnets are ones of dominant sources of impedances in the 3GeV Rapid Cycling Synchrotron (RCS) at Japan Proton Accelerator Research Complex (J-PARC). They may be limiting factors in achieving high intensity beams. Recently, the 300kW beam was accomplished at 3GeV RCS, while no instability was observed. In this paper, the space-charge effects are studied as beam stabilization effects.

 
FR5RFP076 Initial Results of Simulation of a Damping System for Electron Cloud-Driven Instabilities in the CERN SPS feedback, dipole, electron, single-bunch 4713
 
  • J.R. Thompson, J.M. Byrd
    LBNL, Berkeley, California
  • W. Höfle, G. Rumolo
    CERN, Geneva
 
 

Funding: Supported by the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.


Single and multi-bunch instabilities on bunch trains driven by electron clouds have been observed in the CERN SPS for some years. In this paper, we present initial results to implement a damping system in a computer simulation of a single bunch vertical instability using the HEADTAIL code. The code simulates the interaction between a proton bunch and a uniform electron cloud that has built up inside of the beam pipe. In all simulations we use typical SPS parameter sets for three different values of the beam momentum : 26 GeV/c, 55 GeV/c and 120 GeV/c. The feedback is implemented as a corrective kick calculated from the vertical centroid of each slice of the electron bunch with a one turn delay. The bandwidth of the feedback is varied by filtering the slice information along the bunch. Initial results indicate that the instability can be damped with a minimum bandwidth of 300 MHz with a relatively high gain.

 
FR5RFP077 Simulation of a Feedback System for the Attenuation of e-Cloud Driven Instability electron, feedback, emittance, background 4716
 
  • J.-L. Vay, M.A. Furman
    LBNL, Berkeley, California
  • R. De Maria
    BNL, Upton, Long Island, New York
  • J.D. Fox, C.H. Rivetta
    SLAC, Menlo Park, California
  • G. Rumolo
    CERN, Geneva
 
 

Funding: Supported by the US-DOE under Contract DE-AC02-05CH11231 and the US-LHC LARP. Used resources of NERSC, supported by the US-DOE under Contract DE-AC02-05CH11231.


Electron clouds impose limitations on current accelerators that may be more severe for future machines, unless adequate measures of mitigation are taken. Recently, it has been proposed to use feedback systems operating at high frequency (in the GHz range) to damp single-bunch transverse coherent oscillations that may otherwise be amplified during the interaction of the beam with ambient electron clouds. We have used the simulation package WARP-POSINST to study the growth rate and frequency patterns in space-time of the electron cloud driven beam breakup instability in the CERN SPS accelerator with, or without, an idealized feedback model for damping the instability. We will present our latest results and discuss their implications for the design of the actual feedback system.

 
FR5RFP078 Update on Electron-Cloud Simulations Using the Package WARP-POSINST electron, lattice, emittance, dipole 4719
 
  • J.-L. Vay, C.M. Celata, M.A. Furman, M. Venturini
    LBNL, Berkeley, California
  • D.P. Grote
    LLNL, Livermore, California
  • K.G. Sonnad
    FZK, Karlsruhe
 
 

Funding: Supported by the US-DOE under Contract DE-AC02-05CH11231, the US-LHC LARP, and the US-DOE SciDAC program ComPASS. Used resources of NERSC, supported by the US-DOE under Contract DE-AC02-05CH11231.


At PAC05, we presented the package WARP-POSINST for the modeling of the effect of electron clouds on high-energy beams. We present here the latest developments in the package. Three new modes of operations were implemented: 1) “build-up mode” where, similarly to Posinst (LBNL) or Ecloud (CERN), the build-up of electron clouds is modeled in one region of an accelerator driven by a legislated bunch train; 2) “quasi-static mode” where, similarly to Headtail (CERN) or Quickpic (USC/UCLA), the “frozen beam” approximation is used to split the modeling of the beam and the electrons into two components evolving on their respective time scales; and 3) “Lorentz boosted mode” where the simulation is performed into a moving frame where the space and time scales related to the beam and electron dynamics fall in the same range. The implementation of modes (1) and (2) was primary motivated by the need for benchmarking with other codes, while the implementation of mode (3) fulfills the drive toward fully self-consistent simulations of e-cloud effect on the beam including the build-up phase. We also present benchmarking with other codes and selected results from its application to e-cloud effects.

 
FR5RFP079 Recent Observations, Experiments and Simulations of Electron Cloud Buildup in Drift Spaces and Quadrupole Magnets at the Los Alamos PSR electron, quadrupole, diagnostics, beam-losses 4722
 
  • R.J. Macek, R.C. McCrady, L. Rybarcyk, T. Zaugg
    LANL, Los Alamos, New Mexico
  • A. A. Browman
    TechSource, Santa Fe, New Mexico
 
 

Funding: Work supported, in part, by DOE SBIR Grant No. DE-FG02-04ER84105 and CRADA No. LA05C10535 between TechSource, Inc. and the Los Alamos National Laboratory.


Recent beam studies have focused on understanding the main sources and locations of electron clouds (EC) which drive the observed e-p instability at the Los Alamos Proton Storage Ring (PSR). Strong EC signals are observed in drift spaces and quadrupole magnets at PSR which together cover ~65% of the ring circumference. New results making use of two longitudinal barriers to isolate the drift space electron diagnostic provide definitive evidence that most of the drift space EC signal is “seeded” by electrons ejected longitudinally by ExB drifts from adjacent quadrupole magnets. This result can explain why weak solenoids and TiN coatings in several drifts spaces had no effect on the e-p instability threshold. Modeling of EC generation in 3D quadrupoles using a modified version of the POSINST code shows that a sizeable fraction of the electrons generated in the quadrupoles are ejected longitudinally into the adjacent drifts. The experimental findings and simulation results will be presented.

 
FR5RFP082 Sheet Beam Klystron Instability Analysis focusing, cavity, klystron, space-charge 4728
 
  • K.L.F. Bane, C. Adolphsen, A. Jensen, Z. Li, G.V. Stupakov
    SLAC, Menlo Park, California
 
 

Funding: Work supported by the U.S. Department of Energy under contract DE-AC02-76SF00515.


An L-band (1.3 GHz) sheet beam klystron that will nominally produce 10 MW, 1.6 ms pulses is being developed at SLAC for the ILC program. In recent particle-in-cell transport simulations of the 115 kV DC beam through the klystron buncher section without rf drive, a hose-type instability has been observed that is the result of beam noise excitation of transverse modes trapped between the rf cells. In this paper we describe analytical calculations and numerical simulations that were done to study the nature of this instability and explore the required mode damping and changes in the beam focusing to suppress it.

 
FR5RFP083 Measurements, Analysis, and Simulation of Microwave Instability in the Low Energy Ring of KEKB impedance, electron, wakefield, synchrotron 4731
 
  • Y. Cai
    SLAC, Menlo Park, California
  • J.W. Flanagan, H. Fukuma, Y. Funakoshi, T. Ieiri, K. Ohmi, K. Oide, Y. Suetsugu
    KEK, Ibaraki
 
 

Using a streak camera, we measured the longitudinal profiles of a positron bunch in the Low Energy Ring (LER) of KEKB at various currents. The measured charge densities were used to construct a simple Q=1 broadband impedance model. The model with three parameters not only gave an excellent description of longitudinal dynamics for a positive momentum compaction factor but also for the negative ones, including bunch shortening bellow a threshold and bursting modes beyond the threshold. Furthermore, our study indicated that the threshold of microwave instability was about 0.5 mA in bunch current in the LER. At the nominal operating current 1.0 mA, there was a 20% increase of the energy spread. The results of measurement, analysis, and simulations will be presented in this paper.

 
FR5RFP089 Transverse Single Bunch Instability in PEP-X impedance, coupling, synchrotron, single-bunch 4746
 
  • L. Wang, G.V. Stupakov
    SLAC, Menlo Park, California
 
 

A proposed high-brightness synchrotron light source (PEP-X) is under design at SLAC. The 4.5-GeV PEP-X storage ring has four theoretical minimum emittance (TME) cells to achieve the very low emittance and two double-bend achromat (DBA) cells to provide spaces for IDs. Damping wigglers will be installed in zero-dispersion straights to reduce the emittance below 0.1nm. In this paper, we present a preliminary estimation of the threshold of the transverse mode coupling instability(TMCI). Three approaches have been used in the estimation and they agree well with each other.

 
FR5RFP093 BTF Simulations for Tevatron and RHIC with Resistive Wall Wake Field wakefield, emittance, impedance, injection 4755
 
  • V.H. Ranjbar, A.V. Sobol
    Tech-X, Boulder, Colorado
  • H.J. Kim, T. Sen, C.-Y. Tan
    Fermilab, Batavia
 
 

Funding: This work was supported by the US DOE Office of Science, Office of Nuclear Physics, under Grant No.DE-FG02-08ER85183


Recent improvements to BBSIM permit detailed simulations of collective effects due to resistive wall wake fields. We compare results of beam transfer measurements (BTF) in the Tevatron and RHIC with and without the effects of resistive wall wake fields. These are then compared to actual BTF measurements made in both machines and the impact of intensity on our measurements. We also investigate the impact of resistive wall wake fields on various chromaticity measurement approaches.

 
FR5RFP094 Development of a 1.5+0.5 Cell Photoinjector electron, bunching, emittance, cavity 4758
 
  • B.D. O'Shea, A. Fukasawa, J.T. Moody, P. Musumeci, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • L. Faillace
    Rome University La Sapienza, Roma
 
 

We present the status of development of a 1.5+0.5 cell photoinjector run in the blowout regime. LANL Parmela simulation results indicate a near uniform beam of slice energy spread on the order of 500 eV when neglecting thermal effects. We examine the use of an extra half cell to control longitudinal beam growth and compare the system in development with previous 1.6 cell photoinjector designs.

 
FR5RFP096 Simulation Results of Current Filamentation Instability Generated from PWFA Electron Beam plasma, electron, emittance, radiation 4764
 
  • B.A. Allen, P. Muggli
    USC, Los Angeles, California
  • C. Huang
    UCLA, Los Angeles, California
  • T.C. Katsouleas
    Duke University, Durham, North Carolina
  • V. Yakimenko
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by US Department of Energy.


Current Filamentation Instability, CFI, (or Weibel instability) is of central importance for relativistic beams in plasmas for the laboratory, ex. fast-igniter concept for inertial confinement fusion, and astrophysics, ex. cosmic jets. Simulations, with the particle-in-cell code QuickPic, with a beam produced by an RF accelerator show the appearance and effects of CFI. The instability is investigated as a function of electron beam parameters (including charge, transverse size and length) and plasma parameters (density and length) by evaluating the filament currents and magnetic fields. We present simulation results, discuss further simulation refinements, suggest criteria and threshold parameters for observing the presence of CFI and outline a potential future experiment.

 
FR5REP004 A Software Architecture for High Level Applications controls, EPICS, status, optics 4779
 
  • G.B. Shen
    BNL, Upton, Long Island, New York
 
 

Funding: Work performed under auspices of the U.S. Department of Energy under Contract No. DE-AC02-98CH10886 with Brookhaven Science Associates, LLC.


A distributed software architecture for high level applications is under development at the NSLS-II (National Synchrotron Light Source II) project. One of the important issues is to make accelerator simulation model run on a standalone model server. To enhance the capacity of the model server, it is required to have a set of narrow and general API to accommodate various existing tracking codes. A preliminary study for the API development has been started at NSLS-II based on The MMLT (Matlab Middle Layer Toolkit).A new interface is developed for the MMLT to support another simulation engine known as Tracy. A virtual accelerator is also built for the NSLS-II storage ring based on the Tracy code and the EPICS framework. Although we don't have a real machine, we can evaluate and develop our high leval application with the support of virtual accelerator. This paper describes the current status of the software architecture for high level applications.

 
FR5REP006 Visual Scenery Technology Study on Cyclotron and Communication Equipment Operation Simulation cyclotron, controls, electromagnetic-fields, pick-up 4785
 
  • S. Luo, D.B. Liao, S. Liu
    Commanding Communications Academy, Wuhan
  • F. Yang, Z.G. Yin, T.J. Zhang
    CIAE, Beijing
 
 

Under the influence of applications using virtual reality in accelerator R&D, this paper discusses the complete process of developing Communication Equipment Operation Simulation (CEOS) based on Creator/Vega Visual Scenery Simulation Technology, operation rules modeling and solutions to its key problem. The virtual scene model for communication equipment is designed with 3D modeling software MultiGen Creator, especially its DOF technology and Switch node. The basic graphs such as wires are drawn through OpenGL call-back functions. By the virtual scene drive Vega, the application of CEOS comes true. Its simulation example shows greatest traits on building similar simulation system e.g. cyclotron virtual prototyping system as well as virtual cyclotron control system.

 
FR5REP023 Interfacing of Third-Party Accelerator Code with the Lucretia Flight Simulator lattice, controls, extraction, monitoring 4814
 
  • S. Molloy, M.T.F. Pivi, G.R. White
    SLAC, Menlo Park, California
  • Y. Renier
    LAL, Orsay
 
 

The Flight Simulator is a tool used for international collaboration in the writing and deployment of online beam dynamics algorithms. Written as an add-on to the Lucretia tracking software, it allows simulation of a beamline in a control system environment identical to that in the control room. This allows the testing and development of monitoring and correction tools by an international collaboration by making the control system transparent to the user. The native beamline representation are those adopted by Lucretia, so, in order to allow third party software, to interface with this system, it was necessary to develop functionality to convert the lattice to a universal representation. Accelerator Markup Language (AML), and its associated Universal Accelerator Parser (UAP), were used for this purpose. This paper describes the use of the UAP to convert the internal beamline representation to AML, and the testing of this conversion routine using the lattice description of the ATF2 final focus experiment at KEK, Japan. Also described are the inclusion of PLACET and SAD based algorithms using appropriate converters, and tests of these on the ATF2 extraction line.

 
FR5REP024 A Flight Simulator Based Beam Based Alignment Package for ATF2 quadrupole, alignment, sextupole, controls 4817
 
  • S. Molloy, G.R. White, M. Woodley
    SLAC, Menlo Park, California
 
 

The Flight Simulator is a Matlab middleware layer which uses the Lucretia beam tracking engine and a lower level EPICS control system to allow the development of beam control and monitoring algorithms in a simulation environment that appears identical to the that of the control room. The goal of ATF2 is to test a novel compact final final focus optics design intended for use in future linear colliders. The newly designed extraction line and final focus system will be used to produce a 37nm vertical waist from the extracted beam. Alignment of the magnetic elements is of vital importance for this goal and it is expected that beam-based alignment (BBA) techniques will be necessary to achieve the necessary tolerances. This paper describes a package for the beam-based alignment of quadrupole and sextupole magnets in the ATF2 damping ring, extraction line, and final focus system. It brings together several common techniques for the alignment of magnetic elements, and has been implemented as a GUI-based tool that may be used on its own, or integrated with other routines. The design of this package is described, and simulation and beam results are shown.

 
FR5REP035 Reliability Analysis of the LHC Machine Protection System: Analytical Description beam-losses 4847
 
  • S. Wagner, R. Nibali
    ETH, Zurich
  • R. Schmidt, J. Wenninger
    CERN, Geneva
 
 

The design and operation of the LHC Machine Protection System (MPS) implicates the trade-off between machine safety and beam availability, defined by MPS reliability in terms of missed emergency beam dumps and false dumps. A generic methodology, including almost 5000 MPS components modeled as individual objects and Monte Carlo simulation, has proved feasible and useful to address that trade-off*. The resulting MPS reliability numbers allow for the comparison of different system configurations with regard to safety and availability. In search of a solution to reduce the simulation time needed for addressing the rare events involved, an analytical description of the model has been developed. Its numerical solution provides an advanced verification of the simulation results and the basis for a rare event approach. The paper introduces the analytical description and the verification of the reliability numbers resulting from the simulations. It specifies to which extent the simulations can be replaced by the analytical model description and where the latter reaches its limits. Furthermore, the meaning of the analytical description as a basis for simulation time reduction is discussed.


*S.Wagner, Balancing Safety and Availability for an Electronic Protection System, ESREL08; S.Wagner, Reliability Analysis of the LHC Machine Protection System: Terminology and Methodology, EPAC08

 
FR5REP036 Interaction of the Large Hadron Collider 7 TeV/c Proton Beam with a Solid Copper Target target, proton, collider, hadron 4850
 
  • N.A. Tahir
    GSI, Darmstadt
  • V.E. Fortov, I. Lomonosov, A. Shutov
    IPCP, Chernogolovka, Moscow region
  • D.H.H. Hoffmann
    TU Darmstadt, Darmstadt
  • R. Piriz
    Universidad de Castilla-La Mancha, Ciudad Real
  • R. Schmidt
    CERN, Geneva
 
 

When the LHC will work at full capacity, two counter rotating beams of 7 TeV/c protons will be generated. Each beam will consist of 2808 bunches while each bunch will comprise of 1.15x1011 protons. Bunch length will be 0.5 ns whereas two neighboring bunches will be separated by 25 ns . Intensity in the transverse direction will be Gaussian with σ = 0.2 mm. Each beam will carry 362 MJ energy, sufficient to melt 500 kg of Cu. Safety is an extremely important issue in case of such powerful beams. We report two–dimensional numerical simulations of hydrodynamic and thermodynamic response of a solid copper cylinder that is facially irradiated by one of the LHC beams in axial direction. The energy loss of protons in copper is calculated employing the FLUKA code and this data is used as input to a hydrodynamic code, BIG2. Our simulations show that the beam will penetrate up to 35 m into the solid copper target. Since the target is strongly heated by the beam, a sample of High Energy Density (HED) matter is generated. An additional application of the LHC, therefore will be, to study HED matte. This is an improvement of our previous work [Tahir et al., PRL 94 (2005) 135004].

 
FR5REP042 Investigations into the USR "Short Pulse" Operation Mode storage-ring, antiproton, ion, electron 4863
 
  • A.I. Papash
    MPI-K, Heidelberg
  • C.P. Welsch
    Cockcroft Institute, Warrington, Cheshire
 
 

Funding: Work supported by the Helmholtz Association of National Research Centers (HGF) under contract number VH-NG-328 and GSI Helmholtzzentrum für Schwerionenforschung GmbH.


One of the central goals of the Ultra-Low energy Storage Ring (USR) project within the future Facility for Low-energy Antiproton and Ion Research (FLAIR) is to provide very short bunches in the 1-2 nanosecond regime to pave the way for kinematically complete measurements of the collision dynamics of fundamental few-body quantum systems – for the first time on the level of differential cross sections. The “short pulse” operation mode may be split up in two steps: First, the cooled coasting beam of low energy ions will be adiabatically captured by a high harmonic RF cavity (20 MHz) into ~50 ns buckets. Second, the beam will be compressed to very short pulses with a desired width of only 1-2 ns by an RF buncher located 2 m in front of the so-called reaction microscope. To efficiently limit the beam energy spread, RF decompression is then done at after the experiment to avoid beam losses. In this contribution, we present numerical investigations of this very particular operation mode.

 
FR5REP048 Optimization of the Bunch Compressor at BNL NSLS Source Development Laboratory linac, electron, gun, synchrotron 4878
 
  • S. Seletskiy, Y. Hidaka, J.B. Murphy, B. Podobedov, H.J. Qian, Y. Shen, X.J. Wang, X. Yang
    BNL, Upton, Long Island, New York
 
 

At BNL NSLS Source Development Laboratory (SDL) 70MeV electron bunches are compressed by the bunch compressor (BC) consisting of a linac section followed by a 4-magnet chicane. The achievable beam compression is limited by nonlinear beam dynamics in the BC and by coherent synchrotron radiation (CSR) effect. In this report we present a novel beam-based technique of chicane calibration, describe the measurements of CSR effect on the beam in the chicane, and discuss the possible scenarios of the BC optimization.

 
FR5REP051 Design of the Pi-Mode Structure (PIMS) for Linac4 coupling, linac, cavity, impedance 4881
 
  • F. Gerigk, R. Wegner
    CERN, Geneva
 
 

The PIMS will accelerate an H- beam from 100 MeV to 160 MeV, the output energy of Linac4. The cell length is constant within each of the 12 seven-cell cavities, but increases from cavity to cavity according to the increasing beam velocity. Its mechanical design is derived from the five-cell normal conducting LEP cavities, which were in operation at CERN for approximately 15 years. Even though the shunt impedance is around 10% lower than for a Side-Coupled Linac (SCL) operating at 704 MHz, the PIMS has the advantage of using the same RF frequency (352 MHz) as all the other accelerating structures in Linac4, thus simplifying and standardising the linac RF system. Furthermore, the simplified mechanical construction of the PIMS, which uses only 84 cells instead of over 400 for the SCL, also reduces construction costs and tuning effort. In this paper we present the electromagnetic design of the PIMS, including the arguments for the choice of a 5% cell-to-cell coupling factor, the shape of the coupling cells, the dimensioning of the wave-guide ports, and the expected field errors during operation.

 
FR5REP053 Higher Order Modes in the SC Cavities of the SPL HOM, cavity, linac, emittance 4887
 
  • F. Gerigk, M. Schuh, J. Tuckmantel
    CERN, Geneva
  • C.P. Welsch
    KIP, Heidelberg
 
 

In this paper is analysed the influence of Higher Order Modes (HOM) on the operation of the superconducting linac section of the SPL, the Superconducting Proton Linac being designed at CERN. For this purpose, the characteristics of the HOMs in the 2 different beta families (0.65, 0.92 both at 704 MHz) of the SPL are calculated to estimate their effect on the cryogenic system and on the beam stability. For both criteria the maximum external Q of the HOMs is defined.

 
FR5REP054 The Linac4 DTL Prototype: Theoretical Model, Simulations and Low Power Measurements DTL, cavity, linac, coupling 4890
 
  • F. Grespan, G. De Michele, F. Gerigk, S. Ramberger
    CERN, Geneva
 
 

A one meter long hot prototype of the LINAC4 DTL, built in a collaboration with INFN Legnaro, was delivered to CERN in 2008. It was then copper plated at CERN is and is presently prepared for high-power testing at the CERN test stand in SM18. In this paper we present 2D/3D simulations and the first RF low-power measurements to verify the electromagnetic properties of the cavity and to tune it before the high-power RF tests. In particular, the influence of the post couplers was studied in order to guarantee stabilization of the accelerating field during operation. We present an equivalent circuit model of the DTL, together with a comparison of 3D simulations and measurement results for the hot model.

 
FR5REP061 Recent Superconducting CH-Cavity Development cavity, linac, ion, coupling 4911
 
  • M. Busch, M. Amberg, A. Bechtold, F.D. Dziuba, H. Liebermann, H. Podlech, U. Ratzinger
    IAP, Frankfurt am Main
 
 

The superconducting CH-cavity is the first multi-cell drift tube cavity for the low and medium energy range of proton and ion linacs. A 19 cell, beta=0.1 cavity has been developed and tested successfully with gradients of up to 7 MV/m. A piezo based fast tuner system has been developped. First horizontal tests of the cavity in a cryo-module with tuner are presented. Additionally, the construction of a new superconducting 325 MHz 7-gap CH-cavity has started. This cavity has an optimized geometry with respect to tuning possibilities, high power RF coupling and minimized end cell lengths. After low power tests it is planned to test this cavity with a 11.4 MeV/u beam delivered by the Unilac at GSI.

 
FR5REP062 A Beam Transport System for the Frankfurt Funneling Experiment rfq, emittance, ion, ion-source 4914
 
  • P. Kolb, N. Mueller, A. Schempp
    IAP, Frankfurt am Main
 
 

The goal of the Frankfurt Funneling Experiment is to multiply beam currents by merging two low energy ion beams. In an ideal case this would be done without any emittance growth. Our setup consists of two ion sources, a Two-Beam-RFQ accelerator and a multi cell deflector which bends the beams to one common beam axis. Current work is the design of a new beam transport system between RFQ accelerator and deflector. With extended RFQ-electrodes the drift between the Two-Beam-RFQ and the rf-deflector will be minimized and therefor unwanted emittance growth prohibited. First rf measurements with a scaled experiment will be presented.

 
FR5REP065 Mechanical Design of the IFMIF-EVEDA RFQ vacuum, rfq, cavity, coupling 4923
 
  • A. Pepato, F. Scantamburlo
    INFN- Sez. di Padova, Padova
  • M. Comunian, A. Palmieri, A. Pisent, C. Roncolato
    INFN/LNL, Legnaro (PD)
  • E. Fagotti
    Consorzio RFX, Associazione Euratom-ENEA sulla Fusione, Padova
 
 

The IFMIF-EVEDA RFQ is a 9.8 m long cavity, whose working frequency is equal to 175 MHz. In the base line design the accelerator tank is composed of 9 modules flanged together and a pattern of lateral CF100 flanges allows to host the dummy tuners and the couplers, and a pattern of CF 150 flanges the apertures for vacuum pumping manifolds as well. The construction procedure of each module foresees the horizontal brazing of four half –module length electrodes and then the vertical brazing of two brazed assembly. The progresses in the design and engineering phase, as well the description of all the fabrication phases are reported.

 
FR5REP066 RFQ Design Optimisation for PAMELA Injector rfq, ion, proton, acceleration 4926
 
  • M.J. Easton, M. Aslaninejad, S. Jolly, J.K. Pozimski
    Imperial College of Science and Technology, Department of Physics, London
 
 

The PAMELA project aims to design an ns-FFAG accelerator for cancer therapy using protons and carbon ions. For the injection system for carbon ions, an RFQ is one option for the first stage of acceleration. An integrated RFQ design process has been developed using various software packages to take the design parameters for the RFQ, convert this automatically to a CAD model using Autodesk Inventor, and calculate the electric field map for the CAD model using CST EM STUDIO. Particles can then be tracked through this field map using Pulsar Physics’ General Particle Tracer (GPT). Our software uses Visual Basic for Applications and MATLAB to automate this process and allow for optimisation of the RFQ design parameters based on particle dynamical considerations. Initial particle tracking simulations based on modifying the field map from the Front-End Test Stand (FETS) RFQ design have determined the best operating frequency for the PAMELA RFQ to be close to 200 MHz and the length approximately 2.3 m. The status of the injector design with an emphasis on the RFQ will be presented, together with the results of the particle tracking.

 
FR5REP067 Novel Integrated Design Method and Beam Dynamics Simulations for the FETS RFQ Cold Model rfq, emittance, FEL, radio-frequency 4929
 
  • S. Jolly, M.J. Easton, P. Savage
    Imperial College of Science and Technology, Department of Physics, London
  • A.P. Letchford, J.K. Pozimski
    STFC/RAL, Chilton, Didcot, Oxon
 
 

A 4m-long, 324MHz four-vane RFQ, consisting of four coupled sections, is currently being designed for the Front End Test Stand (FETS) at RAL in the UK. Previous beam dynamics simulations, based on field maps produced with a field approximation code, provide a baseline for the new design. A novel design method is presented that combines the CAD and electromagnetic modelling of both the RFQ tank and the vane modulations with more sophisticated beam dynamics simulations using the General Particle Tracer code (GPT). This approach allows the full integration of the optimisation of the RFQ, based on beam dynamics simulations using a 3D EM-field map of the CAD model, with the design and manufacture of the RFQ vane modulations and RFQ tank. The design process within the Autodesk Inventor CAD software is outlined and details of the EM modelling of the RFQ in CST EM Studio are given. Results of beam dynamics simulations in GPT are presented and compared to previous results with field approximation codes. Finally, possible methods of manufacture based on this design process are discussed.

 
FR5REP070 Development of IH Accelerating Structures with PMQ Focusing for Low-Beta Ion Beams focusing, cavity, quadrupole, ion 4938
 
  • S.S. Kurennoy, J.F. O'Hara, E.R. Olivas, L. Rybarcyk
    LANL, Los Alamos, New Mexico
 
 

We are developing high-efficiency room-temperature RF accelerating structures based on inter-digital H-mode (IH) cavities and the transverse beam focusing with permanent-magnet quadrupoles (PMQ), for beam velocities in the range of a few percent of the speed of light. Such IH-PMQ accelerating structures following a short RFQ can be used in the front end of ion linacs or in stand-alone applications such as a compact deuteron-beam accelerator up to the energy of several MeV. New results from our detailed electromagnetic 3-D modeling combined with beam dynamics simulations and thermal-stress analysis for a complete IH-PMQ accelerator tank, including the end-cell design, will be presented.

 
FR5REP071 Simulation of Large Acceptance Linac for Muons linac, acceleration, cavity, proton 4941
 
  • H.M. Miyadera, A.J. Jason, S.S. Kurennoy
    LANL, Los Alamos, New Mexico
 
 

Muon accelerators are proposed world wide for future neutrino factory, muon colliders and other applications. One of the problem on accelerating muons is their large emittance as well as huge energy spreads. We carried out some simulation works on large acceptance muon linear accelerator that operates at mixed buncher / acceleration mode. The designed linac has following features: iris structure of 12 cm diameter, inject ~100 MeV muon beam and accelerates to several 100 MeV, 700 MHz and 25 MV/m peak field. Further acceleration of the muon beam can be easily done by extending the muon linear accelerator. According to the simulation, our linac can accelerates DC muon beam of 20 - 100 MeV range with 20 % phase acceptance.

 
FR5REP072 Use of a Debuncher Cavity for Improving Multi-Beam Operations at LANSCE cavity, DTL, linac, beam-transport 4944
 
  • L. Rybarcyk, S.S. Kurennoy
    LANL, Los Alamos, New Mexico
 
 

Funding: This work is supported by the U. S. Department of Energy, Contract DE-AC52-06NA25396.


The Los Alamos Neutron Science Center simultaneously provides both H- and H+ beams to several user facilities. Opposite polarity beams are usually accelerated in the linac during the same macropulse when beam-loading limitations are not exceeded. Presently, the Weapons Neutron Research (WNR) H- and Isotope Production Facility (IPF) H+ beams are accelerated simultaneously during the same macropulse. The amplitude of the cavity field in the last 201-MHz buncher, located in the common transport just upstream of the DTL, is a compromise between the optimal values for each beam. Recent beam dynamics studies have shown that implementing a debuncher cavity in the H- low-energy beam transport would allow for more optimal operation of both beams. For this application where space is limited, a compact 201-MHz quarter-wave cavity will be used. This paper will report on the beam dynamics simulations performed and the quarter-wave cavity design being developed to address this issue.

 
FR5REP078 A Fourth Order Resonance of a High Intensity Linac resonance, linac, emittance, space-charge 4959
 
  • D. Jeon
    ORNL, Oak Ridge, Tennessee
  • G. Franchetti, L. Groening
    GSI, Darmstadt
 
 

The 4ν=1 resonance of a linac is demonstrated when the depressed tune is around 90 deg. It is observed that this fourth order resonance is dominating over the better known envelope instability and practically replacing it. Simulation study shows a clear emittance growth by this resonance and its stopband. One of the authors [DJ] made a proposal to GSI to measure the stopband of this resonance. The experiment was conducted successfully and the experiment data will be presented separately in the conference.

 
FR5REP079 Design of a 104-MHz Trapezoidal IH-RFQ rfq, impedance, cavity, linac 4962
 
  • Y.C. Nie, J.E. Chen, J.X. Fang, S.L. Gao, Z.Y. Guo, Y.R. Lu, X.Q. Yan, K. Zhu
    PKU/IHIP, Beijing
 
 

Funding: supported by NSFC (19775009)


A trapezoidal IH-RFQ (T-IH-RFQ) is being built to accelerate 14C^+ from 40 keV to 500 keV, motivated by RFQ based 14C AMS application at Peking University. The last design of beam dynamics and the optimized results of RF structure will be presented in this paper. The length of the cavity is about 1.1m operating at {10}4MHz, with a designed transmission efficiency of more than 97%. A special feature is that the RFQ output beam energy spread is as low as 0.6% approached by the method of internal discrete bunching. On the other hand, the new RF cavity structure T-IH-RFQ was proposed for the beam dynamics design, which has higher resonant frequency than traditional four rods RFQ and IH-RFQ at the same transverse dimension. Microwave Studio (MWS) simulations have been performed to study the field distribution and power consumption characteristic of this T-IH-RFQ. The specific shunt impedance and the quality factor have been optimized. Those details will be given.

 
FR5REP080 Commissioning Status of 10-MeV Intense Electron Linac electron, linac, klystron, gun 4965
 
  • S.H. Kim, M.-H. Cho, W. Namkung, H.R. Yang
    POSTECH, Pohang, Kyungbuk
  • S.D. Jang, S.J. Park, Y.G. Son
    PAL, Pohang, Kyungbuk
  • J.-S. Oh
    NFRI, Daejon
 
 

Funding: This work is supported by KAPRA and POSTECH Physics BK21 Program.


An intense L-band electron linac is now being commissioned at ACEP (Advanced Center for Electron-beam Processing in Cheorwon, Korea) for irradiation applications. It is capable of producing 10-MeV electron beams with the 30-kW average beam power. For a high-power capability, we adopted the traveling-wave structure operated with the 2π/3-mode at 1.3 GHz. The structure is powered by a 25-MW pulsed klystron with 60-kW average RF power. The RF pulse length is 8 μs while the beam pulse length is 7 μs due to the filling time in the accelerating structure. The accelerating gradient is 4.2 MV/m at the beam current of 1.45 A which is the fully beam-loaded condition. In this paper, we present details of the accelerator system and commissioning status.

 
FR5REP092 Beam Optics Study on the Extraction Region for a High Intensity Compact Cyclotron extraction, cyclotron, optics, emittance 4993
 
  • S.M. Wei, S. An, M. Li, T.J. Zhang
    CIAE, Beijing
  • Y.-N. Rao
    TRIUMF, Vancouver
 
 

As a high intensity compact cyclotron, CYCIAE-100 is designed to provide proton beams in two directions simultaneously. At the extraction region, the fringe field of the main and the field of the combination magnet will influence the beam optics. The fringe field may become critical by comparison with the separated sector machine because of the compact structure. The dispersion during the beam extraction should not be ignored, which may make the beam envelop become evidently bigger. Then the beam loss and residual radiation increase. To study the beam optics at the extraction region of CYCIAE-100, the orbit tracking and transfer matrix calculation and symplectic by function extension of the code GOBLIN and modification of STRIPUBC have been implemented. The characteristics of the extracted beam have been investigated based on the main field from a FEM code and overlapping with the field generated from the combination magnet at each extraction port. The results are also compared with those from the CIAE’s code CYCTRS to confirm this precise prediction. The transfer matrix from this simulation is analyzed and used for the down stream beam line design.

 
FR5REP095 An Alternative Design for the RACCAM Magnet with Distributed Conductors focusing, beam-transport, magnet-design, hadron 5002
 
  • D. Neuvéglise
    SIGMAPHI S.A., Vannes
  • F. Méot
    CEA, Gif-sur-Yvette
 
 

Funding: ANR contract nb : NT05-141853


This paper presents an alternative design of the magnet for the RACCAM project. The aim of this collaboration is to study and build a prototype of a scaling spiral FFAG as a possible medical machine for hadron therapy. The magnet was first designed with a variable gap to produce the desired field law B=B0(r/r0)^k. The key feature in the “scaling” behavior of the magnet is in getting the fringe field extent to be proportional to the radius. Although the fringe field is increasing with gap dimension, we have obtained quit constant tunes in both horizontal and vertical by using a variable chamfer. An alternative magnet design was then proposed with parallel gap and distributed conductors on the pole to create the required field variation. This solution requires about 40 conductors along the pole and much more power than the gap shaping solution. We expect a much better tune constancy even without variable chamfer. We can think about an “hybrid” magnet with parallel gap at small radii and gap shaping afterward. Such a solution could take advantages of both solutions.

 
FR5REP110 Magnetic Measurements of the RACCAM Prototype FFAG Dipole alignment, dipole, instrumentation, lattice 5032
 
  • M.J. Leray, P. Bocher, B. Diougoant, F. Forest, J.L. Lancelot
    Sigmaphi, Vannes
  • F. Méot
    CEA, Gif-sur-Yvette
  • J. Pasternak
    LPSC, Grenoble
 
 

The paper presents the magnetic measurements of the RACCAM prototype FFAG dipole, manufactured by SIGMAPHI for the Raccam ANR Medical FFAG project. This magnet prototyping work, started early 2006, is being performed in collaboration between the IN2P3/LPSC Laboratory team and SIGMAPHI. This paper describes the magnetic measurement results and comparison with Tosca simulation.

 
FR5REP115 Recent Studies of the FFAG-ERIT System for BNCT neutron, target, emittance, proton 5047
 
  • K. Okabe
    University of Fukui, Faculty of Engineering, Fukui
  • Y. Mori
    KURRI, Osaka
  • M. Muto
    FFAG DDS Research Organization, Tokyo
 
 

The accelerator–based neutron source using ERIT (Energy/emittance Recovery Internal Target) scheme has been constructed at KURRI (Kyoto University Research Reactor Institute). And the first beam test was successfully completed in March 2008. In this poster, recent status of beam studies will be presented.

 
FR5REP123 Beam Commissioning of Separated Function RFQ Accelerator rfq, ion, cavity, ion-source 5071
 
  • J.E. Chen, J.X. Fang, S.L. Gao, J.F. Guo, Z.Y. Guo, M. Kang, W.G. Li, Y.R. Lu, S.X. Peng, Z.Z. Song, Z. Wang, X.Q. Yan, J.X. Yu, M.L. Yu, M. Zhang, K. Zhu
    PKU/IHIP, Beijing
 
 

Funding: work supported by NSFC(10805003,10855001)


The beam commissioning of Separated Function RFQ (SFRFQ) accelerator, which can gain high accelerating efficiency and enough focusing strength for low energy high current beam, is presented. In order to demonstrate the feasibilities of this novel accelerator, a prototype cavity was designed and constructed. The O+ beam was accelerated from 1MeV to 1.6MeV by SFRFQ cavity. A triplet was constructed for the transverse beam matching between the 1MeV ISR-RFQ 1000 and SFRFQ. A capacitance frequency tuning system and RF phase shifter were used to keep SFRFQ cavity working at the same frequency of ISR RFQ at the right phase. The whole RFQ accelerator system and the preliminary beam test results are presented in this paper.