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dipole

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MO1BCI03 Status of LHC Commissioning injection, quadrupole, vacuum, optics 7
 
  • J. Wenninger
    CERN, Geneva
 
 

Beam commissioning of the LHC started with injection tests in August 2008, and a circulating beam was obtained in little over 3 days in September 2008. Unfortunately a powering incident in one the eight LHC sectors set an abrupt end to the beam commissioning in 2008. This talk will review the LHC beam commissioning achievements. It will describe the repair the LHC sector affected by the incident and present the measures that have been taken to avoid similar incidents in the future. The commissioning steps foreseen for the 2009 run and towards LHC design performance will be outlined.

 

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Slides

 
MO6PFP001 Bending Magnets Made with Permanent Magnets for the LNLS-2 Electron Storage Ring electron, permanent-magnet, radiation, storage-ring 127
 
  • G. Tosin, R. Basílio, S. Casas, R.J.F. Marcondes
    LNLS, Campinas
 
 

We present several alternative designs of hybrid bending magnets based on the use of ferrite blocks with steel pole pieces to be used in the new Brazilian storage ring - LNLS2. Their main magnetic and mechanical characteristics are presented. Such models are compared to electromagnet magnets, and some advantages and disadvantages are listed, as well as a cost estimate.

 
MO6PFP004 Small Gap Magnets and Vacuum Chambers for eRHIC vacuum, electron, quadrupole, simulation 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.

 
MO6PFP005 Steering Magnet Design for a Limited Space quadrupole, sextupole, rfq, DTL 136
 
  • M. Okamura, J.M. Fite, V. Lo Destro, D. Raparia, J. Ritter
    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 steering magnet is not a major component in a beam line, however it is usually needed in any real set up. Also it is hard to estimate the required field strength before the beam line construction, since the strength needed is determined by misalignnment errors of other devises. Sometimes it is difficult to find enough space to install steering magnets because of other constraints on the length of the beamline. We compare two extreme designs of steering magnets. The first one is very thin steering magnet design which occupies only 6 mm in length and can be additionally installed as needed. The other is realized by applying extra coil windings to a quadrupole magnet and does not consume any length. We will present both designs in details and will discuss pros and cons.

 
MO6PFP006 Design of the NSLS II High Order Multipole Correctors* sextupole, multipole, quadrupole, controls 139
 
  • M. Rehak, J. Bengtsson, G. Danby, J.W. Jackson, J. Skaritka, C.J. Spataro
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


Feasibility studies for two families of corrector magnets for NSLS-II are presented. The first family of magnets are generalizations of figure eight quadrupoles using rotationally symmetric breaks in the return yoke to fit in available space. Properties specific to figure eight magnet are identified. The second type of magnet is a combined sextupole/dipole trim.

 
MO6PFP008 The Design and Construction of NSLS-II Magnets multipole, quadrupole, sextupole, lattice 145
 
  • J. Skaritka, J. Bengtsson, G. Danby, G. Ganetis, W. Guo, R.C. Gupta, J.W. Jackson, A.K. Jain, S.L. Kramer, S. Krinsky, Y. Li, W. Meng, B. Nash, S. Ozaki, M. Rehak, S. Sharma, C.J. Spataro, F.J. Willeke
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


NSLS-II is a new state-of-the-art medium energy synchrotron light source designed to deliver world leading brightness and flux with top-off operation for constant output. Design and engineering of NSLS-II began in 2005 and the beginning of construction and operations are expected to start in 2009 and 2015, respectively. The energy of the machine is 3Gev and the circumference 792 m. The chosen lattice requires tight on magnetic field tolerances for the ring magnets. These magnets have been designed with 3D Opera software. The required multipole field quality and alignment preclude the use of multifunctional sextupoles, leading to discrete corrector magnets in the storage ring. The corrector magnets are multifunctional and will provide horizontal and vertical steering as well as skew quadrupole. This paper describes the dipoles, quadrupoles, sextupoles, and corrector magnets design and prototyping status of the NSLS-II.

 
MO6PFP009 Design and Measurement of the NSLS II Correctors quadrupole, vacuum, power-supply, storage-ring 148
 
  • G. Danby, J.W. Jackson, A.K. Jain, M. Rehak, O. Singh, J. Skaritka, C.J. Spataro
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


Discrete corrector magnets are used for the 230 horizontal and vertical steering magnets in the NSLS-II storage ring. A unique design incorporates both dipole and skew quad correctors for(DC) steering in the same magnet. Separate AC (orbit feedback) correctors have also been designed. Comparison with alternate designs are presented as well as prototype measurements

 
MO6PFP010 Design and Measurement of the NSLSII Sextupoles sextupole, vacuum, synchrotron, storage-ring 151
 
  • C.J. Spataro, A.K. Jain, M. Rehak, J. Skaritka
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


The Sextupole magnets for the National Synchrotron Light Source (NSLS-II) have stringent performance requirements. These magnets have a faceted pole profile departing from the classic shape due to constraint imposed by the vacuum tube. Three different geometric features were used as parameters to minimize unallowed harmonics. Prototypes were measured and have confirmed the good field quality.

 
MO6PFP015 Fabrication and Production Test Results of Multi-Element Corrector Magnets for the Fermilab Booster Synchrotron booster, sextupole, power-supply, controls 163
 
  • G. Velev, J. DiMarco, C.C. Drennan, D.J. Harding, V.S. Kashikhin, O. Kiemschies, S. Kotelnikov, J.R. Lackey, A.V. Makarov, A. Makulski, R. Nehring, D.F. Orris, W. Pellico, E. Prebys, P. Schlabach, D.G.C. Walbridge
    Fermilab, Batavia
 
 

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


The fabrication of the multi-element corrector magnets for the Fermilab Booster synchrotron has just been completed. These water-cooled packages include six different corrector types - normal and skews oriented dipole, quadrupole and sextupole elements. They will provide full orbit control, tune and chromaticity of the beam over the whole range of Booster energies, from 0.4 GeV to 8 GeV. During production, a set of quality assurance measurements were performed, including special thermal tests. This paper summarizes the results from these measurements as well as discussing some specific steps of the magnet fabrication process.

 
MO6PFP016 Magnetic-Field Calculations for the Magnets of the High-Energy Storage Ring (HESR) at FAIR sextupole, quadrupole, multipole, lattice 166
 
  • H. Soltner, U. Bechstedt, R. Tölle
    FZJ, Jülich
  • J.G. De Villiers
    iThemba LABS, Somerset West
 
 

Funding: Work supported by BMBF and NRF, Project code SUA 06/003


Forschungszentrum Jülich has taken the leadership of a consortium responsible for the design, installation and commissioning of the High-Energy Storage Ring (HESR) for antiprotons as part of the FAIR project at GSI in Darmstadt, Germany. Since a normal-conducting design of the ring has now been favored over the previously envisioned superconducting option, new calculations have been performed in order to assess the magnetic field characteristics of the normal-conducting dipole, quadrupole, and sextupole magnets of the HESR. This paper presents the physical features of the magnets and the results of the 3D calculations with emphasis on the various multipole contributions at the ends of the magnets.

 
MO6PFP017 Magnetic Field Control in Synchrotrons synchrotron, controls, pick-up, quadrupole 169
 
  • A. Peters, E. Feldmeier, R. Steiner
    HIT, Heidelberg
  • H. Eickhoff, T. Knapp, C.P. Welsch
    GSI, Darmstadt
  • C. Schömers
    MPI-K, Heidelberg
 
 

The use of hadron beams delivered by normal conducting synchrotrons is highly attractive in various fundamental research applications as well as in the field of particle therapy. These applications require fast synchrotron operation modes with pulse-to-pulse energy variation and magnetic field slopes up to 10 T/s. The aims are to optimize the duty-cycle or to minimize treatment times for the patients as well as to provide extremely stable properties of the extracted beams, i.e. position and spill structure. Studies performed at the SIS18 synchrotron at GSI showed that not only the dipoles but the quadrupoles as well significantly contribute to the underlying time constants of the slowly extracted beam. An attempt has been made to measure the magnetic fields in synchrotron magnets with high precision and speed comparable to the current measurement with a DCCT. Additional magnetic field monitoring includes the retarding effects into the current control feedback loop neglecting the unfavourable dynamic effects from hysteresis and eddy currents. The presentation describes this controls approach, the results obtained at the HIT synchrotron and the SIS18 at GSI will be discussed.

 
MO6PFP028 Status of Magnet Design for the Accelerator Lattice of the TPS Project quadrupole, sextupole, booster, storage-ring 196
 
  • C.-S. Hwang, C.-H. Chang, H.-H. Chen, M.-H. Huang, J.C. Jan, C.Y. Kuo, F.-Y. Lin, C.-S. Yang
    NSRRC, Hsinchu
 
 

The accelerator lattice magnets of the Taiwan Photon Source (TPS) with energy 3 GeV have been designed for the storage and booster ring. The magnetic computation codes of TOSCA and RADIA software packages were used to design the magnet circuits of the accelerator magnets. Meanwhile, the design of a magnet circuit must take into account both the requirements of accelerator physics and practical engineering constraints. The criterion of magnet design is to keep a rise of coil temperature within 10o C and a safety margin greater than 15 %. We apply pole edge shims and end magnet chamfers to enhance the field homogeneity and to decrease multipole components, respectively. The edge shim involves a smaller magnet dimension but maintains the same quality of the field. Use of an end magnet chamfer avoids field saturation. The mechanical engineering design of the storage ring magnets has been completed and the booster ring magnets have started to be designed. The 3D Solidworks package was used to draw and design the mechanical engineering. The prototype magnets of the storage ring have been contracted out to the local company in Taiwan and will be finished before the end of 2009.

 
MO6PFP030 Development of Combined Function Magnets for the Taiwan Photon Source quadrupole, sextupole, multipole, synchrotron 202
 
  • C.Y. Kuo, C.-H. Chang, C.-S. Hwang
    NSRRC, Hsinchu
 
 

Bending magnets, quadrupole magnets, and sextupole magnets are the most crucial magnetic elements in the synchrotron accelerator facility or high energy accelerator collider ring. Generally, separate bending magnets, quadrupoles or sextupoles magnets are utilized to perform separate functions. However, in the lattice design of accelerator ring or a compact ring in limited space, a single multifunction magnet is used to reduce the number of magnets and ensure that the entire device fits into the available space. This work presents an approach for designing the pole profiles of a combined-function bending magnet of the dipole, quadrupole, and sextupole components. The pole profile of a combined quadrupole magnet with gradient field and sextupole field components is also discussed.

 
MO6PFP032 Magnet System for PLS-II Project quadrupole, sextupole, lattice, septum 208
 
  • D.E. Kim, H.S. Han, H.-G. Lee, K.-H. Park, H.S. Suh, Y.G. Young-Gyu
    PAL, Pohang, Kyungbuk
 
 

Funding: Supported by the MOEST of Korea and by POSCO


Pohang Accelerator Laboratory (PAL) is planning to upgrade the Pohang Light Source (PLS) which is a 3rd generation light source operating since 1995. The key features of the upgrade are, decrease of the beam emittance to 5.6 nm, increasing the beam energy to 3.0 GeV, additional shorter straight sections for more insertion devices. Because the PLSII should use practically same circumference preserving the shielding wall structure of the existing PLS, the lattice space is squeezed to the limit to secure the additional space for the insertion devices. This requirements forces heavy use of the combined function magnet. All dipoles are replaced to gradient magnet, and all sextupoles have horizontal corrector winding, vertical corrector winding, skew quadrupole windings. In this report, the design features and engineering efforts for the PLSII magnet systems are reported.

 
MO6PFP034 Field Distribution of the 90 Degree Bending Magnet of the IFUSP Microtron microtron, electron, booster, linac 214
 
  • C. Jahnke, A.A. Malafronte, M.N. Martins, T.F. Silva, V.R. Vanin
    USP/LAL, Sao Paulo
 
 

Funding: FAPESP, CNPq


The IFUSP Microtron transport line guides the 5 MeV electron beam from the booster to the main microtron, where it can be accelerated up to 38 MeV in steps of 0.9 MeV. A few meters after leaving the main microtron, the beam is guided to the experimental hall, which is located 2.7 m below the accelerator room. The beam leveling is made by two 90° bending magnets. In the experimental hall there is a switching magnet to drive the beam to two different experimental lines. Each of these lines has another 90° bending magnet. These magnets were designed, constructed and characterized. In this work we present the analysis of the field distribution of these 90° bending magnets. Comparison between field simulation and data from field mapping is presented. We also present a reproducibility analysis where the field distributions of two twin magnets are presented.

 
MO6PFP035 Magnetic Measurements of the Booster Dipole Magnets for the ALBA Synchrotron synchrotron, booster, linac, synchrotron-radiation 217
 
  • F. Forest, P. Bocher, B. Diougoant, T. Fevrier, J.L. Lancelot, M.J. Leray
    Sigmaphi, Vannes
  • D. Einfeld, M. Pont
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The paper presents the magnetic measurements of the 32 long dipoles and 8 short dipoles magnet manufactured by Sigmaphi for the ALBA synchrotron booster based in Spain. An extensive set of measurements based on search coils was made by Sigmaphi to characterize the magnetic field at different currents. This paper describes the magnetic measurements results. The measurements show the maximum field integral deviation between the magnets is within ± 3.10-3 as expected.

 
MO6PFP041 Direct Double-Helix Magnet Technology multipole, quadrupole, radiation, laser 229
 
  • R.B. Meinke, J. Lammers, P.J. Masson, G.M. Stelzer
    AML, Palm Bay, Florida
 
 

Magnets for beam steering, focusing and optical corrections often have demanding requirements on field strength, field uniformity, mechanical robustness and high radiation strength. The achievable field strength in normal conducting magnets is limited by resistive heating of the conductor. A break-through magnet technology, called “Direct Double-HelixTM” allows operation at current densities in excess of 100 A/mm2 with conventional water cooling. The conductive path generating the magnetic field is machined out of conductive cylinders, which are arranged as concentric structures. Geometrical constraints of conventional conductors, based on wire manufacturing, are eliminated. The coolant, typically water or air, is in direct contact with the conductor and yields very high cooling efficiency. Based on Double-HelixTM technology the conductor path is optimized for high field uniformity for accelerator magnets with arbitrary multipole order or combined function magnets. Advanced machining technologies, enable unprecedented magnet miniaturization. These magnets can operate at temperatures of several hundred degrees Celsius and can sustain high radiation levels.

 
MO6PFP043 Fabrication of a Prototype of a Fast Cycling Superferric Dipole-Magnet ion, superconductivity, synchrotron, controls 232
 
  • G. Sikler, W. Gaertner, A. Wessner
    BNG, Würzburg
  • E.S. Fischer, E. Floch, D. Krämer, J. Macavei, P. Schnizer, C. Schroeder, F. Walter
    GSI, Darmstadt
 
 

GSI had manufactured a prototype of a fast cycling superconducting dipole magnet at Babcock Noell GmbH. This is the first full size magnet for the SIS100 synchrotron at the future Facility for Antiproton and Ion Research (FAIR) in Darmstadt / Germany. In close collaboration with GSI, the magnet was technologically developed, manufactured and assembled by Babcock Noell. The system was successfully tested at GSI reaching the nominal cycling performance, including the high ramping rate of 4 T/s and the maximum field of 2.1 T. Especially the superconducting cable, the coils and the iron yoke are subject to strong mechanical and thermal stresses. Here we describe the details on the fabrication of these components and give an outlook on possible improvements of the manufacturing technologies, applicable to future prototypes and series magnets for SIS100.

 
MO6PFP046 First Field Test of FiDeL the Magnetic Field Description for the LHC injection, controls, quadrupole, optics 241
 
  • L. Bottura, M.C.L. Buzio, N. Catalan-Lasheras, L. Deniau, M. DiCastro, S.D. Fartoukh, M. Giovannozzi, P. Hagen, J.-P. Koutchouk, M. Lamont, J. Miles, RV. Remondino, N.J. Sammut, S. Sanfilippo, F. Schmidt, D. Sernelius, R.J. Steinhagen, M. Strzelczyk, E. Todesco, R. Tomás, W. Venturini Delsolaro, L. Walckiers, J. Wenninger, R. Wolf, P. Xydi
    CERN, Geneva
 
 

The start-up of the LHC has provided the first field test for the concept, functionality and accuracy of FiDeL, the Field Description for the LHC. FiDeL is primarily a parametric model of the transfer function of the main field integrals generated by the series of magnets in the LHC powering circuits, from main optical elements to high-order harmonic correctors, both superconducting and normal-conducting magnets. In addition, the same framework is used to predict harmonic errors of both static and dynamic nature, and forecast appropriate corrections. In this paper we give a description of the level of detail achieved in the model and the rationale adopted for the LHC start-up. Beam-based measurements have been used for an assessment of the first-shot accuracy in the prediction of the current setting for the main arc magnets*.


*The work reported has been performed by the authors and the FiDeL Team

 
MO6PFP047 Upgrade of the Protection System for Superconducting Circuits in the LHC radiation, instrumentation, interlocks, quadrupole 244
 
  • R. Denz, K. Dahlerup-Petersen, F. Formenti, K.H. Meß, A.P. Siemko, J. Steckert, L. Walckiers
    CERN, Geneva
  • J. Strait
    Fermilab, Batavia
 
 

Prior to the re-start of the Large Hadron Collider LHC in 2009 the protection system for superconducting magnets and bus bars QPS will be submitted to a substantial upgrade. The foreseen modifications will enhance the capability of the system in detecting problems related to the electrical interconnections between superconducting magnets as well as the detection of so-called symmetric quenches in the LHC main magnets. The paper will describe the design and implementation of the new protection layers and report as well on the commissioning of the system and first operational results.

 
MO6PFP049 Methods to Detect Faulty Splices in the Superconducting Magnet System of the LHC cryogenics, quadrupole, superconducting-magnet 247
 
  • J. Strait
    Fermilab, Batavia
  • R. Bailey, M. Bednarek, B. Bellesia, N. Catalan-Lasheras, K. Dahlerup-Petersen, R. Denz, C. Fernandez-Robles, R.H. Flora, E. Gornicki, M. Koratzinos, M. Pojer, L. Ponce, R.I. Saban, R. Schmidt, A.P. Siemko, M. Solfaroli Camillocci, H. Thiesen, A. Vergara-Fernández
    CERN, Geneva
  • Z. Charifoulline
    RAS/INR, Moscow
  • P. Jurkiewicz, P.J. Kapusta
    HNINP, Kraków
 
 

The incident of 19 September 2008 at the LHC was apparently caused by a faulty inter-magnet splice of about 200 nOhm resistance. Cryogenic and electrical techniques have been developed to detect other abnormal splices, either between or inside the magnets. The quench protection system is used in a special mode to measure the voltage across each magnet with an accuracy better than 0.1 mV, allowing internal splices with R > 10 nOhm to be detected. Since this system does not cover the bus between magnets, the cryogenic system is used in a special configuration* to measure the rate of temperature rise due to ohmic heating. Accuracy of a few mK/h, corresponding to a few Watts, has been achieved. This allows detection of excess resistance of more than a few tens of nOhms in a cryogenic sub-sector (2 optical cells). Follow-up measurements, using an ad-hoc system of high-accuracy voltmeters, are made in regions identified by the cryogenic system. These techniques have detected two abnormal internal magnet splices of 100 nOhms and 50 nOhms respectively. In 2009, this ad-hoc system will be replaced with a permanent one which will monitor all splices at the nOhm level.


*L. Tavian, Helium II Calorimetry for the Detection of Abnormal Resistive Zones in LHC Sectors, this conference.

 
MO6PFP053 Study of a Less Invasive LHC Early Separation Scheme luminosity, separation-scheme, emittance, collider 256
 
  • G. Sterbini
    CERN, Geneva
 
 

The LHC Early Separation Scheme consists in a four 5-10 Tm dipole scheme (D0s) installed close to the two LHC high luminosity experiments. Its aim, in the framework of LHC Phase II Upgrade, is to improve the luminosity by reducing the crossing angle between the two colliding beams, mitigating and controlling at the same time their parasitic interactions. We investigate a less invasive implementation in the detectors (D0 at 14 from the IP) with respect to those already presented (D0 at 7 m from the IP). The luminosity performances are discussed and a tentative analysis on beam-beam effect impact is given. For the new D0 position, preliminary dipole design and power deposition results are shown.

 
MO6PFP054 Pre-Cycle Selection for the Superconducting Main Magnets of the Large Hadron Collider injection, coupling, collider, superconducting-magnet 259
 
  • A.P. Verweij, N.J. Sammut, W. Venturini Delsolaro, R. Wolf
    CERN, Geneva
 
 

Pre-cycles for setting up the main magnets of the Large Hadron Collider are necessary for ensuring field reproducibility and low field-decay rates at injection. In this paper we propose standard pre-cycles for the main magnets of the LHC. We study the influence of the pre-cycle parameters on the field decay at injection by two different models. One already proven model is semi-empirical based on magnetic measurements of the magnets. The other is a new network based model of a Rutherford cable which directly calculates the current redistribution and associated magnetization change in the cable strands. The pre-cycle to be used may depend on the history of the machine or may have to be changed because of unforeseen phenomena in the machine. The choice of a new pre-cycle on the basis of magnetic measurements alone is a lengthy process. We confirm the usefulness of the network based model as a tool for selecting new pre-cycles, including decay-blocking degaussing pre-cycles, and compare with magnetic measurements.

 
MO6PFP059 4-Coil Superconducting Helical Solenoid Model for MANX solenoid, quadrupole, simulation, 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.

 
MO6PFP060 Studies of the High-Field Section for a Muon Helical Cooling Channel solenoid, target, beam-cooling, emittance 268
 
  • M.L. Lopes, V.S. Kashikhin, A.V. Zlobin
    Fermilab, Batavia
  • R.P. Johnson, S.A. Kahn
    Muons, Inc, Batavia
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-07ER84825


This paper presents the results of design studies of a high field section of a helical cooling channel proposed for the 6D muon beam cooling. The results include the magnet aperture limitations, the tunability of field components, the field correction, the superconductor choice and the magnet operation margin.

 
MO6PFP061 Solenoid Focusing Lenses for the R&D Proton Linac at Fermilab solenoid, focusing, linac, alignment 271
 
  • M.A. Tartaglia, J. DiMarco, Y. Huang, D.F. Orris, T.M. Page, R. Rabehl, I. Terechkine, J.C. Tompkins, T. Wokas
    Fermilab, Batavia
 
 

Funding: Work supported by the U.S. Department of Energy under contract No. DE-AC02-07CH11359


An R&D proton linac is under construction at FNAL and it will use solenoid lenses in the beam transport line. Because the needed focusing field is on the level of 6 Tesla, superconducting systems are used. In the low energy part of the linac, which uses room temperature accelerating structures, the lenses are placed in stand-alone cryostats. Production of the lenses and cryostats for the low energy section is under way. In the superconducting accelerating sections, the lenses are mounted inside RF cryomodules. Although focusing solenoids for the high energy sections have been designed and prototypes tested, R&D is still ongoing to address magnetic shielding and alignment issues. This report summarizes the performance of lenses for the low-energy part of the linac and presents the status of ongoing R&D.

 
MO6PFP062 RF Integration into Helical Magnet for Muon 6-Dimensional Beam Cooling cavity, solenoid, vacuum, quadrupole 274
 
  • K. Yonehara, V.S. Kashikhin, M.J. Lamm, M.L. Lopes, A.V. Zlobin
    Fermilab, Batavia
  • R.P. Johnson, S.A. Kahn, M.L. Neubauer
    Muons, Inc, Batavia
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-07ER84825 and by FRA under DOE Contract DE-AC02-07CH11359


The helical cooling channel is proposed to make a quick muon beam phase space cooling in a short channel length. The challenging part of the helical cooling channel magnet design is how to integrate the RF cavity into the compact helical cooling magnet. This report shows the possibility of the integration of the system.

 
MO6PFP065 Fast Ramped Superferric Prototype Magnets of the FAIR Project – First Test Results and Design Update multipole, synchrotron, cryogenics, magnet-design 277
 
  • E.S. Fischer, A. Bleile, E. Floch, J. Macavei, A. Mierau, P. Schnizer, C. Schroeder, A. Stafiniak, F. Walter
    GSI, Darmstadt
  • W. Gaertner, G. Sikler
    BNG, Würzburg
 
 

The 100 Tm synchrotron SIS 100 is the core component of the international Facility of Antiproton and Ion Research (FAIR) to be built in Darmstadt. An intensive R&D period was conducted to design 3m long 2T dipoles providing a stable ramp rate of 4 T/s within an usable aperture of 115mm x 60mm with minimum AC losses, high field quality and good long term operation stability. Three full size dipole - and one quadrupole magnets were built. Recently the first dipole magnet, produced by Babcock Noell, was intensively tested at the GSI cryogenic test facility. We present the measured characteristic parameters: training behaviour, the field quality along the load line for DC operation as well as on the ramp, AC losses, and the cryogenic operation limits. We compare them to the calculated results as well as to the requested design performance. Based on the obtained results we discuss adjustments for the final design.

 
MO6PFP067 Magnetic Field Measurements of HD2, a High Field Nb3Sn Dipole Magnet sextupole, multipole, quadrupole, simulation 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.

 
MO6PFP073 PAMELA Magnets - Design and Performance injection, multipole, octupole, proton 301
 
  • H. Witte, J.H. Cobb, T. Yokoi
    OXFORDphysics, Oxford, Oxon
  • K.J. Peach, S.L. Sheehy
    JAI, Oxford
 
 

Funding: This work was supported by EPSRC grant EP/E032869/1.


PAMELA is a design study of a non-scaling FFAG for hadron therapy aiming to deliver 250 MeV protons and 400 MeV/u carbon ions. This paper outlines the general magnet design required for the 250 MeV proton case. The magnet design is challenging because of the combination of required field strength (up to 4T), geometric constraints (the magnets need to be short) and large beam aperture (up to 160 mm). All magnets are combined function magnets with dipole, quadrupole, sextupole and octupole field components of good field quality.

 
MO6PFP088 LCLS Undulator System Tuning and Magnetic Measurements undulator, quadrupole, alignment, electron 336
 
  • Z.R. Wolf, S.D. Anderson, V. Kaplounenko, Yu.I. Levashov, A.W. Weidemann
    SLAC, Menlo Park, California
 
 

The LCLS project at SLAC requires 40 undulators be tuned, fiducialized, and a final data set taken. The techniques used to do this work are presented. In addition, the quadrupoles between the undulators must be accurately fiducialized. A description of the quadrupole magnetic measurements and fiducialization is also presented.

 
MO6RFP002 Status of NSLS-II Storage Ring Vacuum Systems photon, vacuum, multipole, radiation 348
 
  • H.-C. Hseuh, L. Doom, M.J. Ferreira, C. Longo, V. Ravindranath, P. Settepani, S. Sharma, K. Wilson
    BNL, Upton, Long Island, New York
 
 

Funding: Work performed under the auspices of U.S. Department of Energy, under contract DE-AC02-98CH10886


National Synchrotron Light Source II is a 3-GeV, 792-meter circumference, high-flux and high-brightness synchrotron radiation facility being constructed at Brookhaven National Laboratory. The storage ring vacuum chambers are made of extruded aluminium and the bending magnet photons are intercepted at discrete photon absorbers. The design of the storage ring vacuum system will be presented, with emphasis on vacuum chamber design and fabrication, pumping arrangements, photon beam tracking and absorber positioning, and interface with other accelerator systems. The evaluation of the aluminium chamber prototypes and RF shielded bellows will also be described.

 
MO6RFP005 CesrTA Vacuum System Modifications vacuum, electron, photon, synchrotron 357
 
  • Y. Li, X. Liu, V. Medjidzade, M.A. Palmer, D.H. Rice, D. L. Rubin, J.J. Savino
    CLASSE, Ithaca, New York
 
 

Funding: Work supported by the National Science Foundation, the US Department of Energy, and the Japan/US Cooperation Program


In concert with the ILC global design effort, the CESR is being converted into ILC Damping Ring Test Accelerator. The vacuum system is undergoing staged reconfigurations to support both the CesrTA physics goals and the CHESS X-ray sources. Six superconducting wigglers were moved to a sector with zero-dispersion. The sector is densely populated with beam instrumentation and diagnostic devices. A new photon stop chamber will be used to handle the high synchrotron radiation power generated from the SCWs at high positron beam energy. A 12-m long gate-valve isolated straight sector was created in a second location, where many electron-cloud diagnostic chambers will be installed and tested. We also configured two very short sections in the arcs, with additional gate valves, to provide flexibility of exchanging various meter-long test chambers with minimum impact to the operations. Many retarding field analyzers were integrated into the vacuum modifications in SCWs, dipoles, and drifts to study EC growth and suppression techniques. Creating environments where both local and collaborator provided equipment can be easily installed has been a major objective in the modifications.

 
MO6RFP008 Experimental Studies of Carbon Coatings as Possible Means of Suppressing Beam Induced Electron Multipacting in the CERN SPS vacuum, electron, injection, emittance 366
 
  • E.N. Shaposhnikova, G. Arduini, J. Axensalva, E. Benedetto, S. Calatroni, P. Chiggiato, K. Cornelis, P. Costa Pinto, B. Henrist, J.M. Jimenez, E. Mahner, G. Rumolo, M. Taborelli, C. Yin Vallgren
    CERN, Geneva
 
 

Electron cloud build-up is a major limitation for the operation of the SPS with LHC beam above nominal intensity. These beams are envisaged in the frame of the LHC luminosity upgrade and will be available from the new injectors LPSPL and PS2. A series of studies have been conducted in order to identify possible means to suppress electron multipacting by coating the existing SPS vacuum chambers with thin films of amorphous carbon. After a description of the experimental apparatus installed in the SPS, the results of the tests performed with beam in 2008 will be presented.

 
MO6RFP014 Thin Film Coating for the Upgrade of the Ion Synchrotron SIS18 at GSI ion, vacuum, quadrupole, cathode 378
 
  • M.C. Bellachioma, H. Kollmus, A. Krämer, J. Kurdal, H. Reich-Sprenger
    GSI, Darmstadt
  • M. Bender
    LMU, München
 
 

Funding: EU design study, contract 515876, DIRAC-PHASE-1, RP6 SIS 18-2


For the future FAIR facility intensities up to 1012 U28+ ions per second are required. For this purpose the existing heavy ion synchrotron SIS18, which will serve as injector, has to be upgraded. Since the required base pressure is 10-10 Pa, among the different measures undertaken to improve the existing UHV system, the installation of NEG coated magnet chambers is foreseen. Two magnetron sputtering facilities were designed and commissioned at GSI to perform the coating. The characterization of the thin films has been carried out by RBS and XPS. Considering that the vacuum chambers mounted in accelerators undergo several venting-activation cycles, a deep investigation on the NEG aging was performed by ERDA. Fourteen dipole and one quadrupole chambers were coated and installed in the SIS 18, and the replacement of the remaining magnet pipes will follow in the next years. Additionally to overcome the dynamic vacuum instability a collimation system equipped with thin film coated absorbers was successfully tested in 2008. The coating facilities, their operating mode, the results achieved on the thin film characterization, and the ones obtained in the SIS 18 are presented.

 
MO6RFP080 Intense Stopping Muon Beams target, proton, solenoid, simulation 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.

 
TU1RAI01 Special Magnet Designs and Requirements for Next Generation Light Sources quadrupole, sextupole, storage-ring, synchrotron 614
 
  • R.C. Gupta, A.K. Jain
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


This paper will describe the requirements, the design and the prototype test results of the magnets for the new synchrotron radiation source NSLS-II now under construction at BNL. Several innovations have been incorporated in the design, in manufacturing and in the alignment procedures of the magnets. Prototypes of these magnets have been built in industry. A dipole design has been developed with a maximized magnetic length which is longer than the mechanical length. The quadrupole and sextupole magnets of NSLS-II must be aligned and positioned to better than 30 microns, a level never achieved before in such accelerators. The paper will present a brief status of the progress made in the techniques developed to measure and achieve these demanding requirements. Another concern has been the distortion of field quality due to the small (150 mm) axial spacing between the iron-yoke of two adjacent magnets. Calculations (in 3-D) and the result of systematic measurements of the field quality in the presence of other magnets and other machine components in close proximity will be presented.

 

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TU1RAI03 Performance of the LHC Magnet System quadrupole, vacuum, superconducting-magnet, cryogenics 624
 
  • L. Rossi, V. Parma
    CERN, Geneva
 
 

The LHC magnet system has been largely commissioned in 2007-08: all sectors up to 7 kA (4 TeV proton beam energy); six (out of eight) sectors were commissioned up 9.3 kA (5.5 TeV) and one to 11.5 kA (6.9 TeV). For more than one week, both beams have been injected, circulated and captured in the RF bucket, thus assessing the optics at injection energy. The incident in sector 3-4, originated by a serious defect of a high-current joint between magnets with large collateral damage, has changed the plans: magnets in the damaged zone (about 50) are being substituted or repaired meanwhile a campaign of consolidation is under way. During commissioning, the training of the main dipoles was longer than expected on the basis of reception tests of individual magnets , thus pointing to a partial loss of quench memory. The thermal performance is within heat losses estimates and the spectacular easiness of the first injection test on 10th September has demonstrated the very good field quality, precise understanding of magnetic characteristics, quality of the elaborate field modeling and the very good shape of the magnets with proper alignment of the machine.

 

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TU1PBI01 Fully 3D Multiple Beam Dynamics Processes Simulation for the Tevatron simulation, proton, beam-beam-effects, 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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TU1PBI03 Monte Carlo Mean Field Treatment of Microbunching Instability in the FERMI@Elettra First Bunch Compressor FEL, emittance, impedance, laser 636
 
  • G. Bassi
    Cockcroft Institute, Warrington, Cheshire
  • G. Bassi
    The University of Liverpool, Liverpool
  • J.A. Ellison, K.A. Heinemann
    UNM, Albuquerque, New Mexico
  • R.L. Warnock
    SLAC, Menlo Park, California
 
 

Microbunching can cause an instability which degrades beam quality. This is a major concern for free electron lasers where very bright electron beams are required. A basic theoretical framework for understanding this instability is the 3D Vlasov-Maxwell system. However, the numerical integration of this system is computationally intensive. Investigations to date have used simplified analytical models or numerical solvers based on simple 1D models. We have developed an accurate and reliable 2D Vlasov-Maxwell solver which we believe improves existing codes. This solver has been successfully tested against the Zeuthen benchmark bunch compressors. Here we apply our self-consistent, parallel solver to study the microbunching instability in the first bunch compressor system of FERMI@Elettra.

 

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TU3GRC05 Commissioning and Performance of LCLS Cavity BPMs cavity, undulator, FEL, alignment 754
 
  • S.R. Smith, S. Hoobler, R.G. Johnson, T. Straumann, A. Young
    SLAC, Menlo Park, California
  • R.M. Lill, L.H. Morrison, W.E. Norum, N. Sereno, G.J. Waldschmidt, D.R. Walters
    ANL, Argonne
 
 

Funding: Work supported by U.S. Department of Energy under Contract Nos. DE-AC02-06CH11357 and DE-AC02-76SF00515.


We present the performance of the cavity beam position monitor (BPM) system for the LCLS undulator. The construction and installation phase of 34 BPMs for the undulator and 2 for the transport line have been completed. The X-band cavity BPM employs a TM010 monopole reference cavity and a TM110 dipole cavity designed to operate at a center frequency of 11.384 GHz. The signal processing electronics features a low-noise single-stage three-channel heterodyne receiver that has selectable gain and a phase locking local oscillator. The approximately 40 MHz IF is digitized by a 120M sample/second four-channel 16-bit digitizer. System requirements include sub-micron position resolution for a single-bunch beam charge of 200 pC. We discuss the system specifications and commissioning results.

 

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TU4PBI01 Emittance Exchange Results emittance, cavity, coupling, space-charge 773
 
  • R.P. Fliller
    Fermilab, Batavia
  • T.W. Koeth
    Rutgers University, The State University of New Jersey, Piscataway, New Jersey
 
 

Funding: This manuscript has been authored by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


The promise of next-generation light sources depends on the availability of ultra-low emittance electron sources. One method of producing low transverse emittance beams is to generate a low longitudinal emittance beam and exchange it with a large transverse emittance. Experiments are underway at Fermilab's A0 Photoinjector and ANL's Argonne Wakefield Accelerator using the exchange scheme of Kim and Sessler. Experiments as the A0 photoinjector exchange a large longitudinal emittance with a small trasverse emittance. AWA expects to exchange a large transvserse emittance with a small logitudinal emittance. In this paper we discuss recent results at A0 and AWA and future plans for these experiments.

 

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TU5PFP006 Wakefield Damping for the CLIC Crab Cavity cavity, damping, wakefield, HOM 815
 
  • P.K. Ambattu, G. Burt, R.G. Carter, A.C. Dexter
    Cockcroft Institute, Lancaster University, Lancaster
  • V.A. Dolgashev
    SLAC, Menlo Park, California
  • R.M. Jones, V.F. Khan
    UMAN, Manchester
 
 

Funding: The work is supported by STFC


A crab cavity is required in the CLIC to allow effective head-on collision of bunches at the IP. A high operating frequency (X-band) for the crab cavity is preferred as the deflection voltage required and the RF phase tolerance are inversely proportional to the operating frequency. However, the strong inter-bunch wakefields deteriorate the quality of the colliding bunches. The short bunch spacing of the CLIC scheme and the crab cavity's high sensitivity to dipole kicks demands very high damping of the inter-bunch wakes. A crab cavity requires special attention to the damper design as its wakefield spectrum is entirely different from that of an accelerating cavity. In addition to the higher-order modes, the orthogonally polarised dipole mode (same order mode) and the fundamental monopole mode (lower order mode) also need to be damped, however their resonant frequencies make damping these modes complicated. The same order mode suppression requires the use of an azimuthally asymmetric damper. This paper investigates the nature of the wakefields in the CLIC crab cavity and the possibility of using choke-mode damping and various types of waveguide damping to suppress them effectively.

 
TU5PFP007 Investigation of an Alternate Means of Wakefield Suppression in the Main Linacs of CLIC wakefield, coupling, damping, linac 818
 
  • V.F. Khan, R.M. Jones
    UMAN, Manchester
 
 

Here we present initial results on an alternate design for CLIC main accelerating linacs which is moderately damped and detuned structure. In order to suppress the wake-fields, we detune the lowest dipole modes as they have significant impact on the beam emittance compared to the other multipoles. In order to mitigate the reappearance of the wake-field of a detuned accelerator structure, we provide moderate damping by coupling cells to manifolds which run parallel to each accelerator structure. The manifolds are designed such that they are non-propagating at the acceleration mode frequency. The cell parameters are optimised by considering the r.f. breakdown, pulse surface heating and beam dynamics constraints.

 
TU5PFP040 Novel Geometries for the LHC Crab Cavity cavity, damping, HOM, radio-frequency 909
 
  • B.D.S. Hall, G. Burt
    Cockcroft Institute, Lancaster University, Lancaster
  • R. Calaga
    BNL, Upton, Long Island, New York
  • J.R. Delayen, R.A. Rimmer, H. Wang
    JLAB, Newport News, Virginia
  • J.D.A. Smith
    Lancaster University, Lancaster
 
 

In 2017 the LHC is envisioned to increase is luminosity via an upgrade. This upgrade is likely to require a large crossing angle hence a crab cavity is required to align the bunches prior to collision. There are two possible schemes for crab cavity implementation, global and local. In a global crab cavity the crab cavity is far from the IP and the bunch rotates back and forward as it traverses around the accelerator in a closed orbit. For this scheme a two cell elliptical squashed cavity at 800 MHz is preferred. To avoid any potential beam instabilities all the modes of the cavities must be damped strongly, however crab cavities have lower order and same order modes in addition to the usual higher order modes and hence a novel damping scheme must be used to provide sufficient damping of these modes. In the local scheme two crab cavities are placed at each side of the IP two start and stop rotation of the bunches. This would require crab cavities much smaller transversely than in the global scheme but the frequency cannot be increased any higher due to the long bunch length of the LHC beam. This will require a novel compact crab cavity design.

 
TU5PFP048 Robustness of the Superconducting Multicell Cavity Design for the Cornell Energy Recovery Linac cavity, HOM, linac, damping 933
 
  • M. Liepe, G.Q. Stedman, N.R.A. Valles
    Cornell University, Ithaca, New York
 
 

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


Cornell University is developing an Energy-Recovery-Linac driven x-ray light source. One of the major components of this accelerator will be its 5 GeV superconducting main linac. The design of the superconducting RF cavities in this main linac has been optimized primarily for two objectives: (1) low RF losses from the accelerating mode to minimize refrigeration cost and (2) strong Higher-Order-Mode damping to preserve low emittance and prevent beam break-up at high beam current (100 mA). In this paper we study the robustness of this optimized cavity design with respect to small cell shape fluctuations from fabrication errors.

 
TU5PFP051 Superconducting Multicell Cavity Design for the Energy Recovery Linac at Cornell cavity, HOM, linac, damping 939
 
  • V.D. Shemelin, M. Liepe
    CLASSE, Ithaca, New York
 
 

Funding: DOE


The first phase of the Cornell Energy Recovery Linac was the high current, low emittance injector. At present the injector is under commissioning. The next phase calls for the development of multicell cavity for the main linac. The cavities need to have low RF losses to minimize refrigeration and strong HOM damping to preserve low emittance and prevent beam break-up at high current (100 mA). Here we present the RF design of the cavity meeting these requirements.

 
TU5PFP064 SC Crab Cavity with Reduced Transverse Size for the LHC Upgrade cavity, HOM, impedance, damping 975
 
  • V.P. Yakovlev, I.G. Gonin, T.N. Khabiboulline, N. Solyak
    Fermilab, Batavia
 
 

In the paper the Crab Cavity is described for local Crab schemes for LHC that demand reduced transverse cavity dimensions small enough to fit limited space necessary for the beams separation. The results of the configuration cavity optimization are presented that include (a) the surface field minimization; (b) parasitic monopole and dipole spectrum optimization and dumping, (c) the input and the parasitic mode damping couplers design. The results of multipacting simulations, which were performed in order to understand the possible gradient limitations, are discussed also.

 
TU5RFP003 Superconducting Multi-Cell Deflecting Cavity for Short-Pulse X-Ray Generation at the Advanced Photon Source cavity, damping, impedance, photon 1087
 
  • G.J. Waldschmidt, L.H. Morrison, R. Nassiri
    ANL, Argonne
  • R.A. Rimmer, K. Tian, H. Wang
    JLAB, Newport News, Virginia
 
 

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 multi-cell cavity for the production of short x-ray pulses at the Advanced Photon Source (APS) has been explored as an alternative to a single-cell cavity design in order to improve the packing factor and potentially reduce the number of high-power RF systems and low-level RF controls required. The cavity will operate at 2815 MHz in the APS storage ring and will require heavy damping of parasitic modes to maintain stable beam operation. Novel on-cell dampers, attached directly to the cavity body, have been utilized by taking advantage of the magnetic field null on the equatorial plane in order to enhance damping. Design issues and simulation results will be discussed.

 
TU5RFP010 Flexibility in the Design of the NSLS-II Lattice emittance, lattice, quadrupole, sextupole 1108
 
  • S.L. Kramer, W. Guo
    BNL, Upton, Long Island, New York
 
 

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


The NSLS-II light source is a proposed 3 GeV storage ring, with the potential for ultra-low emittance*. The lattice design uses a 30 cell DBA structure with a periodicity of 15, for alternating long and short straight sections. All cells are tuned achromatic to maximize the emittance reduction achieved as damping wigglers are added to the ring. Recent optimization of the lattice consisted of increasing the number of possible hard X-ray beam ports using three pole wigglers, reducing the number of magnets (quadrupoles and sextupoles) and shifting the magnets to allow easier extraction of the photon beams. The impact of the reduction of magnets on the lattice flexibility will be presented in terms of the tuning range possible for the lattice parameters: tune, emittance, and chromaticity, beta function matching to user insertion devices (IDs) and for compensating for ID induced distortions to these parameters. This flexibility is important for optimizing the lattice linear and nonlinear properties, the dynamic aperture, and its impact on beam lifetime, as well as matching the user source requirements and for value engineering of magnets and power supplies.


*Work presented on behalf of the NSLS-II Design Team, CDR(2006), CD2(2007) and CD3(2008).

 
TU5RFP011 Top-Off Safety Analysis for NSLS-II simulation, 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.

 
TU5RFP025 A Full-Energy-Injector for the ANKA Storage Ring storage-ring, optics, injection, quadrupole 1147
 
  • E. Huttel, I. Birkel, A.-S. Müller, N.J. Smale, K.G. Sonnad, P. Wesolowski
    FZK, Karlsruhe
 
 

The ANKA storage ring is filled at 0.5 GeV and then ramped to 2.5 GeV for regular user operation. A full-energy injection of the ANKA storage ring would have several advantages. The damping at a beam energy of 2.5 GeV is stronger, which will more efficiently fight instabilities during the injection, therefore allowing higher beam currents. With constant magnet settings, the orbit stability would improve significantly. The injection time would be reduced and topping- up operation would become possible. As a consequence, the optical elements of the user beamlines would see a constant power as a function of time which further enhances the overall stability. In this paper, a design for a full energy injector is proposed. The injector will be located inside the storage ring tunnel, similar to the SLS and ALBA design. The focusing is mainly provided by combined function magnets. The full energy injector has a design emittance of 40 nmrad and a circumference of 94.8 m. A modification of the existing storage ring is foreseen to house the necessary more powerful injection elements.

 
TU5RFP048 Design and Performance of Linac and Recirculation Optics for the X-Ray Free Electron Laser Oscillator emittance, linac, optics, quadrupole 1195
 
  • 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.


The X-ray Free Electron Laser Oscillator* (XFEL-O) is a concept for a high-brightness fourth-generation x-ray source with full spatial and temporal coherence. It is based on a CW electron source and superconducting linac. In order to reduce cost and increase versatility, a recirculating linac configuration is being entertained. In this paper, we present an optics design for the four-pass linac and the three recirculation systems. The design goals are preservation of the beam emittance and energy spread, as well as minimal cost and complexity. We also present the results of tracking studies that show the expected performance.


*K.J. Kim et al., Phys. Rev. Letters, to be published.

 
TU5RFP080 Multi-Beam Injection and Quasi-CW ERL for Future X-Ray Light Sources linac, cavity, emittance, septum 1275
 
  • 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.


The envisioned next-generation ERL-based x-ray light sources demand costly CW superconducting linacs and high-brightness high-current photoinjectors that are beyond the state of the art. To overcome the fiscal challenge of a multi-GeV CW superconducting ERL and the physical challenge of high-brightness high-current CW photoinjectors, we explore a new scheme using multi-beam injection into a quasi-CW ERL. Multi-beam injection lowers the burden on individual rf injectors at subharmonics of the linac frequency. Lower injector frequency allows higher bunch charge, which permits lower duty factor of the linac with significant reduction in construction and operation costs. Preliminary studies foresee many benefits and no obvious physical showstoppers, despite potential technical challenges. Here we provide a simulation study of a preliminary design.

 
TU6PFP028 GENEPI-3C, a Versatile Neutron Generator for the GUINEVERE ADS Feasibility Studies target, extraction, emittance, neutron 1348
 
  • J.-M. De Conto, M.A. Baylac, A. Billebaud, P. Boge, D. Bondoux, J. Bouvier, T. Cabanel, Y. Carcagno, G. Dargaud, E. Froidefond, Y. Gómez-Martínez, M. Heusch, D. Marchand, R. Micoud, E. Perbet, M. Planet, D. Tourres
    LPSC, Grenoble
  • P. Beaten, G. Vittiglio
    SCK-CEN, Mol
  • G. Gaudiot, G. Heitz, P. Poussot, C. Ruescas
    IPHC, Strasbourg Cedex 2
  • J.M. Gautier, Y. Merrer
    LPC, Caen
  • G. Granget, F. Mellier
    CEA Cadarache, Saint Paul Lez Durance
  • J. Laune, D. Reynet
    IPN, Orsay
 
 

GUINEVERE, Generator-of-Uninterrupted-Intense-NEutrons-at-the-lead-VEnus-REactor, is devoted to ADS feasibility studies and to investigate on-line reactivity monitoring, sub-criticality determination and operational procedures. It will couple a versatile neutron source to the VENUS-F lead core at the SCK·CEN site in Mol (Belgium). It is based on an electrostatic accelerator generating 14 MeV neutrons by bombarding a deuteron beam on a tritium target located in the reactor core. A new accelerator has been developed. It will produce alternatively 1 μs 250 keV deuteron pulses with adjustable repetition rate (40 mA peak), as well as continuous beam (1 mA) with programmable interruptions. Beam will be inserted vertically into the reactor core. The accelerator is designed to enable the vertical section of the beam line to be easily lifted out the reactor bunker for maintenance operations, target changes and core loading procedures. This paper will describe the design of the accelerator and its commissioning in Grenoble (France), before its transfer to the Belgian site. This work is performed within the 6th Framework Program EC project EUROTRANS.

 
TU6PFP040 A Compact Ring for Thom X-Ray Source cavity, HOM, emittance, impedance 1372
 
  • C. Bruni, Y. Fedala, J. Haissinski, M. Lacroix, B. Mouton, R. Roux, A. Variola, Z.F. Zomer
    LAL, Orsay
  • E. Bressi
    CNAO Foundation, Milan
  • P. Brunelle, M.-E. Couprie, J.-C. Denard, N. Guillotin, P. Lebasque, A. Loulergue, P. Marchand, F. Marteau, R. Nagaoka
    SOLEIL, Gif-sur-Yvette
  • P. Gladkikh
    NSC/KIPT, Kharkov
 
 

The goal of X-ray sources based on Compton back scattering processes is to develop a compact device, which could produce an intense flux of monochromatic X-rays. Compton back-scattering resuls from collisions between laser pulses and relativistic electron bunches. Due to the relative low value of the Compton cross section, a high charge electron beam, a low emittance and a high focusing at the interaction point are required for the electron beam. In addition, the X-ray flux is related to the characteristics of the electron beam, which are themselves dynamically affected by the Compton interaction. One possible configuration is to inject frequently into a storage ring with a low emittance linear accelerator without waiting for the synchrotron equilibrium. As a consequence, the optics should be designed taking into account the characteristics of the electron beam from the linear accelerator. The accelerator ring design for a 50 MeV electron beam, aiming at producing a flux higher than 1013 ph/s, will be presented.

 
TU6PFP049 Coherent Terahertz Radiation Emitted by Sub-Picosecond Electron Bunches in a Magnetic Chicane radiation, electron, simulation, polarization 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.

 
TU6PFP088 Chopper for Intense Proton Beams at Repetition Rates up to 250 kHz high-voltage, kicker, proton, neutron 1500
 
  • C. Wiesner, L.P. Chau, M. Droba, N.S. Joshi, O. Meusel, I. Müller, U. Ratzinger
    IAP, Frankfurt am Main
 
 

A chopper system for high intensity proton beams of up to 200 mA and repetition rates up to 250 kHz is under development at IAP to be tested and applied at the Frankfurt Neutron Source FRANZ. The chopper system consists of a fast kicker for transversal separation of the beams and a static septum magnet to lower the dynamic deflection angle. Multi-particle simulations and preliminary experiments are presented. The simulations were made using a Particle in Cell (PIC)-Code developed at IAP. It permits the study of collective effects of compensation and secondary electrons on the proton beam in time-dependent kicker fields. A magnetic kicker with high repetition rate would entail high power consumption while electrostatic deflection in combination with intense beams can lead to voltage breakdown. Therefore a Wien filter-type ExB configuration consisting of a static magnetic dipole field and a pulsed electric field to compensate the magnetic deflection is discussed. The 25 kV high voltage pulser (250 kHz, 100 ns) will apply fast MOSFET transistor technology in the primary circuit, while the high voltage is provided at the secondary circuit around a metglas transformer core.

 
TU6RFP011 Increasing Output Current Stability by Adding an External Current Control Loop controls, power-supply, feedback, booster 1556
 
  • K.-B. Liu, C.Y. Wu
    NSRRC, Hsinchu
 
 

The Agilient 6682A power supply is used as a dipole magnet power supply of Booster to storage ring (BTS) transport line, its output current stability is less than 100 ppm although specification is 1000 ppm. The performance of Agilient 6682A is quite good for TLS operational requirement but not suitable for less than 10 ppm output current stability general requirement of power supplies of TPS. Circuitry modification of Agilient 6682A to reach less than 10 ppm output current stability is hard to implement; but utilize analog programming function of Agilient 6682A with adding an external current control loop the output current stability of Agilient 6682A could be improved to less than 10 ppm.

 
TU6RFP019 Elettra Booster Magnet Power Supplies: One Year of Operations power-supply, booster, storage-ring, extraction 1571
 
  • R. Visintini, D.M. Molaro
    ELETTRA, Basovizza
 
 

The New Full-Energy Injector at Elettra, based on a 3 Hz, 100 MeV to 2.5 GeV booster has officially started its operations since March 2008*. The time schedule was fully respected notwithstanding the performance problems presented by some of the main magnet power supplies**. The refurbishing plan, formally started at the end of the commissioning phase and carried on together with the manufacturer, has brought positive results in approaching the required specifications. The paper will describe the progress of the refurbishing and the experience with the other magnet power supplies, including the positive performances of the in-house low-current (5A) bipolar power supplies, especially designed for the linac pre-injector***. A new version, fully digitally controlled, of these low-power power supplies will be adopted for some coils and magnets of the FERMI@Elettra project.


*M. Svandrlik, Status of the Elettra Booster Project, EPAC08
**R. Visintini, Magnet power converters for the Elettra Booster, EPAC08
***D. Molaro, A new bipolar PS for the Elettra booster, PCIM08

 
TU6RFP020 Magnet Power Supplies for FERMI@Elettra power-supply, FEL, quadrupole, electron 1574
 
  • R. Visintini, M. Cautero, D.M. Molaro
    ELETTRA, Basovizza
 
 

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


FERMI@Elettra is the new 4th-generation light source, based on a single-pass FEL, under construction at the Elettra Laboratory in Trieste, Italy. Some hundreds of magnets and coils need to be supplied along the accelerator sections and the undulators chains - mostly individually - with currents as low as 1.5 A up to 750 A. Starting from a successful design developed at Elettra* for the full-energy injector**, a new version of the existing 4-quadrant, 5 A PS has been studied. This new bipolar low-current PS, with full digital control, will be adopted for all 1.5 A and 5 A loads. The design of a bipolar PS for supplying the 20 A loads is in progress. This paper will describe the proposed PS system for the magnets and coils of FERMI@Elettra. The focus will be on the solutions adopted to minimize the number of different PS types. Particular stress will be laid upon the in-house design.


*D, Molaro et al. - A new bipolar power supply for Elettra booster pre-injector correctors - PCIM08
**R. Visintini et al. - Magnet power converters for the new Elettra full energy injector - EPAC08

 
TU6RFP028 Laser Stripping for the PS2 Charge-Exchange Injection System laser, resonance, emittance, injection 1596
 
  • B. Goddard, W. Bartmann
    CERN, Geneva
  • V.V. Danilov
    ORNL, Oak Ridge, Tennessee
  • D.E. Johnson
    Fermilab, Batavia
 
 

Laser stripping for an H- injection system into the proposed PS2 accelerator could provide an attractive alternative to the use of a conventional stripping foil. In this paper possible concepts for a 4 GeV laser stripping system are outlined and compared, using either laser or magnetic initial stripping steps and a resonant excitation of the intermediate H0 atom, followed by a final magnetic stripping. Issues of laser power, overall efficiency and emittance growth are discussed.

 
TU6RFP033 AC Dipole System for Inter-Bunch Beam Extinction in the Mu2e Beam Line proton, simulation, 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.

 
TU6RFP038 Conceptual Design of Beam Transport Lines for the PEFP User Facility proton, target, quadrupole, optics 1626
 
  • B.-S. Park, Y.-S. Cho, B.H. Choi, I.-S. Hong, J.-H. Jang, H.S. Kim, K. R. Kim, H.-J. Kwon, H.R. Lee, S.P. Yun
    KAERI, Daejon
 
 

Funding: This work is supported by the Ministry of Education, Science and Technology of Korea.


PEFP (Proton Engineering Frontier Project) beamlines will be supplied either 20-MeV or 100-MeV proton beams from the 100-MeV proton linear accelerator for beam applications. Each proton beam will be transported to 2 beamlines for industrial purpose and 3 beamlines for the researches. Beam distribution to 3 research beam lines will be conducted sequentially by programmable AC magnet. To provide flexibility of the irradiation conditions, each beam line is designed to have specific beam parameters. We have designed the beamlines to the targets for wide or focused beams, external or in-vacuum beams, and horizontal or vertical beams. The detail design of each beamline will be reported.

 
TU6RFP045 Stored Beam Stability during Pulsed Sextupole Injection at the Photon Factory Storage Ring injection, photon, factory, sextupole 1647
 
  • H. Takaki, N. Nakamura
    ISSP/SRL, Chiba
  • K. Harada, T. Honda, Y. Kobayashi, T. Miyajima, S. Nagahashi, T. Obina, M. Shimada, A. Ueda
    KEK, Ibaraki
 
 

We successfully demonstrated a new beam injection method using a single pulsed sextupole magnet (PSM). The PSM has a parabolic-shaped magnetic field, which is expected to provide an effective kick to the injected beam without little effects on the stored beam. We installed the PSM injection system at the Photon Factory storage ring (PF-ring) and succeeded in injecting the beam into PF-ring and storing the current up to 450 mA. This is the first demonstration of the PSM beam injection in electron storage rings. We also tested top-up injection and confirmed that dipole oscillation of the stored beam was sufficiently reduced compared with that generated by the conventional injection system. In this conference, we will present the experimental results and the advantages of the PSM beam injection.

 
WE1PBC05 Development of an Ultra-High Repetition Rate S-Band RF Gun for the SPARX Project gun, coupling, FEL, quadrupole 1815
 
  • L. Faillace, L. Palumbo
    Rome University La Sapienza, Roma
  • P. Frigola
    RadiaBeam, Marina del Rey
  • A. Fukasawa, B.D. O'Shea, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • B. Spataro
    INFN/LNF, Frascati (Roma)
 
 

We present here the design, including RF modelling, cooling, and thermal stress and frequency detuning, of an S-band RF gun capable of running near 500 Hz, for application to FEL and inverse Compton scattering sources. The RF design philosophy incorporates many elements in common with the LCLS gun, but the approach to managing cooling and mechanical stress diverges significantly. We examine the new proprietary approach of RadiaBeam Technologies for fabricating copper structures with intricate internal cooling geometries. We find that this approach may enable very high repetition rate, well in excess of the nominal project this design is directed for, the SPARX FEL.


*C.Limborg et al.,“RF Design of the LCLS Gun”,LCLS Technical Note LCLS-TN-05-3
**P. Frigola et al.,“A Novel Fabrication Technique for the Production of RF Photoinjectors”,published in EPAC08.

 

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WE4RAC04 Power Supply System for SESAME Booster booster, injection, kicker, septum 1944
 
  • S. Varnasseri, A. Nadji
    SESAME, Amman
 
 

The SESAME booster, with a circumference of 38 m, has several bending magnets, focussing quadrupoles and defocussing quadrupoles and also the injection and extraction septums and kickers. There wil be one ramping power converter which supplies a series of 12 dipole magnets. Also 12 focussing magnets family and 6 defocussing magnets family are supplied separately with two ramping power converters. Technical issues of all the ramping and pulsed power supplies needed for the SESAME booster are disussed in this paper.

 
WE4GRC05 Machine Protection for the Experiments of the LHC proton, injection, beam-losses, interlocks 1976
 
  • R. Appleby, D. Macina
    CERN, Geneva
 
 

The LHC stored beam contains 362 MJ of energy at the top beam energy of 7 TeV, presenting a significant risk to the components of the machine and the detectors. In response to this threat, a sophisticated system of machine protection has been developed to minimize the danger, and detect potentially dangerous situations. In this paper, the protection of the experiments in the LHC from the machine is considered, focusing on pilot beam strikes on the experiments during injection and on the dynamics of hardware failure with a circulating beam, with detailed time-domain calculations performed for LHC ring power converter failures and magnet quenches. The prospects for further integration of the machine protection and experimental protection systems are considered,along with the risk to near-beam detectors from closed local bumps.

 

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Slides

 
WE5PFP054 HOM Survey of the First CEBAF Upgrade Style Cavity Pair cavity, HOM, impedance, cryomodule 2123
 
  • F. Marhauser, E. Daly, G.K. Davis, M.A. Drury, C. Grenoble, J. Hogan, R. Manus, J.P. Preble, C.E. Reece, R.A. Rimmer, K. Tian, H. Wang
    JLAB, Newport News, Virginia
 
 

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


For the planned CEBAF upgrade ten new cryomodules are required to increase the beam energy to the envisaged 12 GeV. Extensive cavity and cryomodule R&D has been done previously, including the installation of a new cryomodule dubbed “Renascence” in CEBAFs north linac in 2007. It houses both seven-cell low loss and high gradient type of cavities thereby serving as a testbed to address and cope with crucial technological challenges. Based on this experience a final iteration on the upgrade cavity has been performed to improve various aspects of HOM-damping and thermal stability. Two such cavities have been produced and qualified. A thorough cavity HOM-survey has been performed to verify the integrity of the cavities and to guarantee the impedance requirements of each crucial HOM. This paper details the results of HOM-surveys performed for the first two upgrade style low loss cavities tested both individually in a vertical Dewar and horizontally in a dedicated cavity pair cryomodule. The safety margin to the worst beam break-up scenario at 12 GeV has been concluded.

 
WE5PFP079 The Damping of Longitudinal Quadrupole Oscillations at GSI damping, quadrupole, controls, cavity 2195
 
  • M. Mehler, H. Klingbeil, M. Kumm, U. Laier, K.-P. Ningel
    GSI, Darmstadt
 
 

Funding: Project funded by the European Community under the FP6 "Structuring the European Research Area" program (SIS1002, contract number 515873)


SIS100 is a synchrotron that will be built in the scope of the FAIR (Facility for Antiproton and Ion Research) project. High intensity ion beams are required, making it necessary to damp longitudinal coupled and uncoupled bunch oscillations. For this purpose, a closed-loop control system was designed. Its processing part is based on digital signal processors (DSP) and field programmable gate arrays (FPGA) whose advantage is their adaptability to different problems by software changes. Experiments with a prototype were performed at the existing synchrotron SIS12/18 at GSI concentrating on the damping of longitudinal coupled bunch quadrupole oscillations of the lowest order. The configuration of the electronic system is described and results of the machine development experiments are reported. Finally, an outlook to the application in SIS100 is given.

 
WE5PFP096 Damping Effect Studies for X-Band Normal Conducting High Gradient Standing Wave Structures damping, acceleration, coupling, impedance 2237
 
  • S. Pei, V.A. Dolgashev, Z. Li, S.G. Tantawi, J.W. Wang
    SLAC, Menlo Park, California
 
 

Funding: Work supported by the DOE under contract DE-AC02-76SF00515.


The Multi-TeV colliders should have the capability to accelerate low emittance beam with high rf efficiency, X-band normal conducting high gradient accelerating structure is one of the promising candidate. However, the long range transverse wake field which can cause beam emittance dilution is one of the critical issues. We examined effectiveness of dipole mode damping in three kinds of X-band, π-mode standing wave structures at 11.424GHz with no detuning considered. They represent three damping schemes: damping with cylindrical iris slot, damping with choke cavity and damping with waveguide coupler. We try to reduce external Q factor below 20 in the first two dipole bands, which usually have very high (RT/Q)T. The effect of damping on the acceleration mode is also discussed.

 
WE5RFP006 Progress Report of the TPS Lattice Design booster, sextupole, quadrupole, lattice 2273
 
  • C.-C. Kuo, H.-P. Chang, H.C. Chao, P.J. Chou, G.-H. Luo, H.-J. Tsai
    NSRRC, Hsinchu
 
 

A 3 GeV synchrotron light source is planned to be built at the existing site of NSRRC campus. The project is called the Taiwan Photon Source (TPS). It will provide x-ray photon beam with brilliance several orders higher than the one generated by the existing 1.5 GeV synchrotron. The design issues of accelerator lattice for the 3 GeV storage ring and booster injector will be presented. These issues cover the properties of linear and nonlinear beam dynamics, the optimization of dynamic aperture and momentum acceptance, collective beam instabilities and lifetime issues, the effects caused by various error sources and technical measures to suppress these error effects, etc.

 
WE5RFP017 Prospect of an IR or THz Beamline at SSRL radiation, synchrotron, synchrotron-radiation, vacuum 2303
 
  • X. Huang, J.A. Safranek
    SLAC, Menlo Park, California
 
 

A preliminary plan for an infrared or terahertz beamline at SSRL is studied. Using chicane in a straight section allows us to redesign a section of the vacuum chamber and extract infrared/terahertz beam with a large acceptance. Under the low alpha operational mode, the terahertz beam power can be greatly enhanced by the coherent synchrotron radiation (CSR) effect. Calculations of photon beam flux and brightness and the shielding and CSR effects are presented.

 
WE5RFP018 Reduction of Beam Emittance of PEP-X Using Quadruple Bend Achromat Cell emittance, damping, brightness, undulator 2306
 
  • M.-H. Wang, Y. Cai, R.O. Hettel, Y. Nosochkov
    SLAC, Menlo Park, California
 
 

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


SLAC National Accelerator Laboratory is studying an option of building a high brightness synchrotron light source machine, PEP-X, in the existing PEP-II tunnel*,**. By replacing 6 arcs of FODO cells of PEPII High Energy Ring (HER) with two arcs of DBA and four arcs of TME and installation of 89.3 m long damping wiggler an ultra low beam emittance of 0.14 nm-rad (including intra-beam scattering) at 4.5 GeV is achieved. In this paper we study the possibility to further reduce the beam emittance by releasing the constraint of the dispersion free in the DBA straight. The QBA (Quadruple Bend Achromat) cell is used to replace the DBA. The ratio of outer and inner bending angle is optimized. The dispersion function in the non-dispersion straight is controlled to compromise with lower emittance and beam size at the dispersion straight. An undulator of period length 23 mm, maximum magnetic field of 1.053 T, and total periods of 150 is used to put in the 30 straights to simulate the effects of these IDs on the beam emittance and energy spread. The brightness including all the ID effects is calculated and compared to the original PEP-X design.


*R. Hettel et al., “Ideas for a Future PEP-X Light Source”, EPAC08, p.2031(2008).
**M-H Wang et al., “Lattice Design of PEP-X as a Light Source Machine at SLAC”, EPAC08, p.2127(2008).

 
WE5RFP041 First Results of the LCLS Laser-Heater System laser, electron, undulator, FEL 2358
 
  • P. Emma, R.F. Boyce, A. Brachmann, R. Carr, F.-J. Decker, Y.T. Ding, D. Dowell, S.A. Edstrom, J.C. Frisch, A. Gilevich, G.R. Hays, P. Hering, Z. Huang, R.H. Iverson, Yu.I. Levashov, H. Loos, A. Miahnahri, H.-D. Nuhn, B.D. Poling, D.F. Ratner, J.L. Turner, J.J. Welch, W.E. White, Z.R. Wolf, J. Wu
    SLAC, Menlo Park, California
  • S. Spampinati
    ELETTRA, Basovizza
 
 

Funding: Work supported by the U.S. Dept. of Energy contract #DE-AC02-76SF00515.


The Linac Coherent Light Source (LCLS) is an x-ray Free-Electron Laser (FEL) project presently in a commissioning phase at SLAC. The very bright electron beam required for the FEL is also susceptible to a micro-bunching instability* in the magnetic bunch compressors, prior to the FEL undulator. The uncorrelated electron energy spread can be increased by an order of magnitude to provide strong Landau damping against the instability without degrading the free-electron laser performance. To this end, a ‘laser-heater’ system has been installed in the LCLS injector, which modulates the energy of a 135-MeV electron bunch with an IR laser beam in a short undulator, enclosed within a four-dipole chicane. The last half of the chicane time-smears the energy modulation leaving an effective thermal energy spread increase. We present the first commissioning results of this system, its operational issues, and its impact on the micro-bunching instability.


*Z. Huang et. al., Phys. Rev. ST Accel. Beams 7, 074401 (2004).

 
WE5RFP043 Optics Design for a Soft X-Ray FEL at the SLAC A-Line linac, emittance, undulator, lattice 2364
 
  • H. Geng, Y.T. Ding, P. Emma, Z. Huang, Y. Nosochkov, M. Woodley
    SLAC, Menlo Park, California
 
 

Funding: This work is supported by the Department of Energy contract DE-AC02-76SF00515.


LCLS capabilities can be significantly extended with a second undulator aiming at the soft x-ray spectrum (1- 5 nm). To allow for simultaneous hard and soft x-ray operations, 14 GeV beams at the end of the LCLS accelerator can be intermittently switched into the SLAC A-line (the beam transport line to End Station A) where the second undulator may be located. In this paper, we discuss the A-line optics design for transporting the high-brightness LCLS beams using the existing tunnel. To preserve the high brightness of the LCLS beams, special attentions are paid to effects of incoherent and coherent synchrotron radiation. Start-to-end simulations using realistic LCLS beam distributions are carried out.

 
WE5RFP044 Tolerance Study for the Echo-Enabled Harmonic Generation Free Electron Laser FEL, bunching, laser, undulator 2367
 
  • D. Xiang, G.V. Stupakov
    SLAC, Menlo Park, California
 
 

Funding: This work was supported by US DOE contracts DE-AC03-76SF00515


The echo-enabled harmonic generation free electron laser (EEHG FEL) holds great promise in generation of coherent soft x-ray directly from a UV seed laser within one stage. The density modulation in the harmonic generation process is affected by the smearing effect caused by the fluctuations of energy and current along the beam, as well as the field error of the dispersive elements. In this paper we study the tolerance of the EEHG FEL on beam quality and field quality.

 
WE5RFP047 A Recirculating Linac as a Candidate for the UK New Light Source Project linac, FEL, laser, cryomodule 2376
 
  • P.H. Williams, D. Angal-Kalinin, J.K. Jones, B.D. Muratori, S.L. Smith
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • R. Bartolini
    JAI, Oxford
  • I.P.S. Martin, J. Rowland
    Diamond, Oxfordshire
  • H.L. Owen
    UMAN, Manchester
  • P.H. Williams
    Cockcroft Institute, Warrington, Cheshire
 
 

A design for a free electron laser driver which utilises 1.3 GHz superconducting CW accelerating structures is studied. The machine will deliver longitudinally compressed electron bunches with repetition rates of 1 kHz with a possibility to increase up to 1 MHz. Tracking is performed from an NC RF photocathode gun, accelerating and compressing in three stages to obtain peak current greater than 1 kA at 2.2 GeV. This is achieved through injection at 200 MeV, then recirculating twice in a 1 GeV main linac. The optics design, optimisation procedures and start to end modelling of this system are presented.

 
WE5RFP084 Spectral Characterisation of the ANKA-SCU Radiation undulator, radiation, electron, simulation 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, simulation, electron 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.

 
WE6PFP006 Overview of Magnetic Nonlinear Beam Dynamics in RHIC sextupole, resonance, lattice, dynamic-aperture 2489
 
  • Y. Luo, M. Bai, J. Beebe-Wang, J. Bengtsson, R. Calaga, W. Fischer, A.K. Jain, N. Malitsky, S. Peggs, F.C. Pilat, V. Ptitsyn, G. Robert-Demolaize, T. Satogata, S. Tepikian, D. Trbojevic
    BNL, Upton, Long Island, New York
  • R. Tomás
    CERN, Geneva
 
 

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


In the article we review the nonlinear beam dynamics from nonlinear magnetic fields in the Relativistic Heavy Ion Collider. The nonlinear magnetic fields include the magnetic field errors in the interaction regions, chromatic sextupoles, and sextupole component from arc dipoles. Their effects on the beam dynamics and long-term dynamic apertures are evaluated. The online measurement and correction methods for the IR nonlinear errors, nonlinear chromaticity, and horizontal third order resonance are reviewed. The overall strategy for the nonlinear effect correction in the RHIC is discussed.

 
WE6PFP041 Petavac: 100 TeV Proton-Antiproton Collider in SSC Tunnel luminosity, collider, synchrotron, lattice 2585
 
  • P.M. McIntyre, A. Sattarov
    Texas A&M University, College Station, Texas
 
 

Funding: DOE grant DE-FG02-06ER41405.


A conceptual design is presented for a 100 TeV proton-antiproton collider consisting of a single storage ring based upon 16.5 T dipoles, installed in the 83 km circumference SSC tunnel, fed using a proportionately expanded antiproton source. Provisions have been designed to intercept synchrotron light on room-temperature photon stops and to suppress electron cloud effect using a continuous clearing electrode running throughout the collider. Beams would be separated using split dipoles so that 20 ns bunch spacing should be attainable. Synchrotron damping time of half-hour would help to stabilize against mechanisms for slow emittance growth. It is reasonable to project the potential for a luminosity of 1035/cm2/s.

 
WE6PFP054 Polarized Beams in the SuperB High Energy Ring sextupole, solenoid, dynamic-aperture, electron 2619
 
  • W. Wittmer, M.H. Donald, Y. Nosochkov, U. Wienands, G. Yocky
    SLAC, Menlo Park, California
  • M.E. Biagini, P. Raimondi
    INFN/LNF, Frascati (Roma)
  • A.V. Bogomyagkov, I. Koop, S.A. Nikitin
    BINP SB RAS, Novosibirsk
 
 

The proposed SuperB factory will provide longitudinal polarized electrons to the experiment. Vertically polarized electrons will be injected into the High Energy Ring; the vertical spin orientation will be locally rotated into the longitudinal direction before the interaction point and back afterwards to avoid spin depolarization. The spin rotators can be designed using compensated solenoids–-as proposed by Zholents and Litvinenko–-to rotate the spin into the horizontal plane, followed by dipoles for horizontal spin rotation into the longitudinal direction. Such spin rotators have been matched into the existing lattice and combined with the crab-waist IR. Several ways of achieving this are explored, that differ in the degree of spin matching achieved and the overall geometry of the interaction region. The spin rotation can also be achieved by a series of dipole magnets only, which present a different optical matching problem. We will compare the different scenarios leading up to the adopted solution.

 
WE6PFP059 Interaction Region Design for a RHIC-Based Medium-Energy Electron-Ion Collider radiation, electron, synchrotron, ion 2634
 
  • C. Montag, J. Beebe-Wang, B. Parker, D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

As first step in a staged approach towards a RHIC-based electron-ion collider, installation of a 4 GeV energy-recovery linac in one of the RHIC interaction regions is currently under investigation. To minimize costs, the interaction region of this collider has to utilize the present RHIC magnets for focussing of the high-energy ion beam. Meanwhile, electron low-beta focussing needs to be added in the limited space available between the existing separator dipoles. We discuss the challenges we are facing and present the current design status of this e-A interaction region.

 
WE6PFP076 CLIC Drive Beam Frequency Multiplication System Design linac, injection, emittance, sextupole 2673
 
  • C. Biscari, D. Alesini, A. Ghigo, F. Marcellini
    INFN/LNF, Frascati (Roma)
  • J.B. Jeanneret
    CERN, Geneva
 
 

The CLIC drive beam current, produced by the 1 GHZ fully loaded Linac, will be multiplied by a factor of 24 by the frequency multiplication system, to generate the high power beam representing the CLIC power source. The frequency multiplication system is composed by one delay loop plus two combiner rings. All rings will be isochronous, will contain trajectory tuning wigglers, and all magnets will be normal conducting. The design of the rings, with special emphasis on the rf deflectors characteristics, is presented.

 
WE6PFP095 Integrating the MANX 6-D Muon Cooling Experiment with the MICE Spectrometers solenoid, emittance, cavity, simulation 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.

 
WE6PFP097 Pulsed Magnet Arc Designs for Recirculating Linac Muon Accelerators linac, quadrupole, superconducting-magnet, acceleration 2733
 
  • G.M. Wang, K.B. Beard, R.P. Johnson
    Muons, Inc, Batavia
  • S.A. Bogacz
    JLAB, Newport News, Virginia
  • G.M. Wang
    ODU, Norfolk, Virginia
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-08ER86351


We have previously considered the application of fast pulsing quadrupoles to increase the focusing of muon beams as they gain energy in the linac region of a recirculating linear accelerator (RLA) in order to allow more passes. In this work we consider the use of pulsed magnets, both quads and dipoles, to reduce the number of beam lines needed for the return arcs of the RLA. We investigate the required relationships between the linac parameters (length and energy gain) and the momentum acceptance of the return arcs and consider the optimum strategy for accelerating both muon charge signs.

 
WE6PFP107 Design Considerations for the CLIC Pre-Damping Rings emittance, wiggler, damping, lattice 2760
 
  • F. Antoniou
    National Technical University of Athens, Zografou
  • Y. Papaphilippou, F. Zimmermann
    CERN, Geneva
 
 

The CLIC pre-damping rings have to accommodate a large emittance beam, coming in particular from the positron target and reduce its size to low enough values for injection into the main damping rings. In particular, polarized positron stacking imposes stringent requirements with respect to longitudinal acceptance and damping times. Linear lattice design options based on low-emittance cells, multiple bend cells and the inclusion of damping wigglers are compared with respect to linear optics functions, tunability, chromatic properties and acceptance. The optics of special regions for the placement of injection, extraction and RF elements are also presented. Non-linear dynamics simulations are finally undertaken for evaluating and maximizing the rings dynamic aperture, especially for large momentum spreads.

 
WE6PFP108 Beam Based Calibration of Slow Orbit Bump at NSLS Booster extraction, booster, septum, simulation 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.

 
WE6PFP111 The First Two Years of Operation of the 1.5 GeV CW Electron Accelerator MAMI C linac, microtron, extraction, electron 2772
 
  • A. Jankowiak, K. Aulenbacher, O. Chubarov, M. Dehn, H. Euteneuer, R.G. Heine, P. Jennewein, H.-J. Kreidel, U. Ludwig-Mertin, O. Ott, G.S. Stephan, V. Tioukine
    IKP, Mainz
 
 

Funding: Work supported by DFG (CRC443) and the German Federal State of Rheinland-Pfalz


In December 2006 the maximum output energy of the cw race track microtron cascade MAMI B was increased to 1508MeV by the successful commissioning of the world wide first Harmonic-Double-Sided-Microtron (HDSM)* as a new fourth stage. Since then MAMI C was in operation for more than 15000 hours, delivering approx. 10000 hours the maximum beam energy of 1508MeV. We will report about our operational experiences and the recent machine developments concerning e.g. the increase of the energy and stabilisation of the output energy down to 10-6. Topics of machine reliability and stability will be addressed and the operation under different demands of nuclear physics experiments described.


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

 
WE6RFP003 Helium II Calorimetry for the Detection of Abnormal Resistive Zones in LHC Sectors cryogenics, quadrupole, superconducting-magnet, superconductivity 2784
 
  • L.J. Tavian
    CERN, Geneva
 
 

Following the incident on a LHC sector due to an electrical arc on the main dipole bus-bar circuit, post-mortem analysis of previous current plateaus has shown abnormal temperature drift in the helium II baths of some magnets in the concerned area. In order to identify other possible risky areas, a detection system based on calorimety using available precision cryogenic thermometers has been first validated by applying calibrated heating in the magnet cold-mass and then implemented in the different sectors. On the 3-km long continuous helium II cryostat of each LHC sector, this method allows detecting abnormal dissipations in the W-range , i.e. additional resistive heating due to abnormal resistance of about 20 nΩ at 7 kA and less than 10 nΩ at nominal current. The paper describes the principle and the methodology of this calorimetric method and gives the results obtained on the LHC sectors.

 
WE6RFP018 Energy Deposition Studies for the LHC Insertion Region Upgrade Phase-1 quadrupole, luminosity, proton, insertion 2820
 
  • F. Cerutti, F. Borgnolutti, A. Ferrari, A. Mereghetti, E.H.M. Wildner
    CERN, Geneva
 
 

While the Large Hadron Collider (LHC) at CERN is starting operation with beam, aiming to achieve nominal performance in the shortest term, the upgrade of the LHC interaction regions is actively pursued in order to enhance the physics reach of the machine. Its first phase, with the target of increasing the LHC luminosity to 2-3 1034 cm-2 s-1, relies on the mature Nb-Ti superconducting magnet technology and is intended to maximize the use of the existing infrastructure. The impact of the increased power of the collision debris has been investigated through detailed energy deposition studies, considering the new aperture requirements for the low-beta quadrupoles and a number of other elements in the insertions. Effective solutions in terms of shielding options and design/layout optimization have been envisaged and the crucial factors have been pointed out.

 
WE6RFP027 Performance of and Upgrades to the SNS Collimator Systems beam-losses, neutron, target, proton 2847
 
  • M.A. Plum, A. Abdou, P.D. Ferguson, P.J. Geoghegan, L.L. Jacobs, J.G. Janney, S.M. McTeer, I.I. Popova, A.P. Zhukov
    ORNL, Oak Ridge, Tennessee
 
 

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


As the SNS beam power is increased, the collimator systems are becoming correspondingly more important. The High Energy Beam Transport (HEBT) transverse collimators are now routinely used during neutron production. We are in the process of redesigning the HEBT momentum collimation system due to problems with gas production from radiolysis. The Ring collimators are designed for two-stage operation but to date they are mainly used in one-stage mode. In this paper we will discuss the status, the operational performance, and upgrades to the collimation systems.

 
WE6RFP049 Optimisation of the Powering Tests of the LHC Superconducting Circuits extraction, quadrupole, simulation, cryogenics 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.

 
WE6RFP081 Design of Advanced Photonic Bandgap (PBG) Structures for High Gradient Accelerator Applications damping, simulation, 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 damping, simulation, 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.

 
WE6RFP094 Preliminary Study of the Arc for a Muon Collider with 1.5TeV CM Energy and Using 20T HTS Dipole Magnets collider, lattice, superconductivity, luminosity 3016
 
  • D.B. Cline, X.P. Ding
    UCLA, Los Angeles, California
  • R.C. Gupta
    BNL, Upton, Long Island, New York
  • R.J. Weggel
    Particle Beam Lasers, Inc., Northridge
 
 

We describe preliminary study of the design of a Muon Collider using 20T Dipole Magnets such a collider could be constructed at FNAL.

 
WE6RFP101 Two-Screen Method for Determining Electron Beam Energy and Deflection from Laser Wakefield Acceleration electron, laser, plasma, wakefield 3035
 
  • B.B. Pollock, J.S. Ross, G.R. Tynan
    UCSD, La Jolla, California
  • C.E. Clayton, C. Joshi, K.A. Marsh, A.E. Pak, T.-L. Wang
    UCLA, Los Angeles, California
  • L. Divol, D.H. Froula, S.H. Glenzer, V. Leurent, J. Palastro, J.E. Ralph
    LLNL, Livermore, California
 
 

We present experimental results showing the formation of a laser produced optical waveguide, suitable for laser guiding, when applying a high external magnetic field around a gas cell. This technique is directly applicable to wakefield acceleration and has been established at the Jupiter Laser Facility; an external magnetic field prevents radial heat transport, resulting in an increased electron temperature gradient [D. H. Froula et.al., Plasma Phys. Control. Fusion, 51, 024009 (2009)]. Interferometry and spatially resolved Thomson-scattering diagnostics measure the radial electron density profile, and show that multiple-centimeter long waveguides with minimum electron densities of 1017 to 1018 cm-3 can be produced. Temporally resolved Thomson-scattering is also performed to characterize the evolution of the density channel in time. This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344 and was partially funded by the Laboratory Directed Research and Development Program under project tracking code 06-ERD-056.

 
TH1GRI02 Status of the China Spallation Neutron Source Project power-supply, injection, linac, rfq 3053
 
  • S. Fu, H. Chen, Y.W. Chen, Y.L. Chi, C.D. Deng, H. Dong, L. Dong, S.X. Fang, W. He, K.X. Huang, W. Kang, X.C. Kong, J. Li, H.F. Ouyang, Q. Qin, H. Qu, C. Shi, H. Sun, J. Tang, S. Wang, J. Wei, T. Wei, T.G. Xu, Z.X. Xu, X. Yin, J. Zhang, Z.H. Zhang
    IHEP Beijing, Beijing
 
 

CSNS accelerator mainly consists of an H- linac and a proton rapid cycling synchrotron. It is designed to accelerate proton beam pulses to 1.6 GeV kinetic energy at 25 Hz repetition rate, striking a solid metal target to produce spallation neutrons. The accelerator is designed to deliver a beam power of 120 kW with the upgrade capability up to 500 kW, The CSNS accelerator is the first large-scale, high-power accelerator project to be constructed in China and thus we are facing a lot of challenges in some key technologies. A series of R&D for major prototypes have being conducted since 2006, including an H- ion source, DTL tank, RF power supply for the linac, injection/extraction magnets and its pulse power supplies, dipole and quadrupole prototype magnets in the ring and its power supplies, ferrite-loaded RF prototype cavity, ceramic vacuum chamber, control and some beam diagnostics. This paper will briefly introduce the design and R&D status of the CSNS accelerator.

 

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TH1GRI04 Overview of the Accelerator Programs at the Indian Laboratories cavity, controls, linac, booster 3059
 
  • V.C. Sahni
    RRCAT, Indore (M.P.)
 
 

Particle accelerator programs being pursued by the Indian labs cover a broad range, encompassing accelerators for nuclear physics research (NPR) (in the low and intermediate energy range), construction of synchrotron radiation sources (SRS) as well as participation in international accelerator projects, especially those related to high energy physics. Machines for NPR include 14MV Pelletrons, augmented by home built superconducting linac boosters to enhance the energy & mass range of the ion beams, and a superconducting cyclotron which is currently undergoing commissioning at Kolkata. Two SRS, namely, a 450 MeV ring Indus-1 and 2.5 GeV booster cum light source, Indus-2, have been indigenously constructed and set up at Indore. A program is also on to develop a high current proton accelerator that will eventually be used for R&D linked to ADS. Regarding our international collaborations, Indian labs have contributed to setting up of LHC at CERN, are associated with the CLIC Test Facility 3 & Linac-4 and the FAIR project at Hamburg besides working with Fermilab on ILC/Project-X R&D. The talk will give an overview of some of the recent developments related to these activities.

 

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TH2PBC02 Nonlinear Dynamics Studies in the Fermilab Tevatron Using an AC Dipole sextupole, octupole, betatron, synchrotron 3073
 
  • R. Miyamoto
    BNL, Upton, Long Island, New York
  • A. Jansson, M.J. Syphers
    Fermilab, Batavia
  • S.E. Kopp
    The University of Texas at Austin, Austin, Texas
 
 

An AC dipole magnet produces a sinusoidally oscillating dipole field with frequency close to betatron frequency and excites large sustained oscillations of beam particles circulating in a synchrotron. Observation of such oscillations with beam-position-monitors allows direct measurements of a synchrotron's nonlinear parameters. This paper presents experimental studies to measure effects of sextupole and octupole fields, such as tune dependence on amplitude and resonance driving terms, performed in the Fermilab Tevatron using an AC dipole.

 

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TH3GAI01 Electron Beam Dynamics in the Long-Pulse, High-Current DARHT-II Linear Induction Accelerator electron, simulation, 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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TH5PFP002 Simulation of Electron Cloud Density Distributions in RHIC Dipoles at Injection and Transition and Estimates for Scrubbing Times electron, injection, simulation, 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.

 
TH5PFP018 Recent Advances in the Synergia Accelerator Simulation Framework simulation, space-charge, impedance, optics 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, simulation, proton, 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.

 
TH5PFP032 Status of Electron-Cloud Build-Up Simulations for the Main Injector simulation, 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.

 
TH5PFP045 SRF Cavity Geometry Optimization for the ILC with Minimized Surface E.M. Fields and Superior Bandwidth cavity, wakefield, higher-order-mode, HOM 3300
 
  • I.R.R. Shinton, R.M. Jones, N. Juntong
    UMAN, Manchester
 
 

The main linacs of the ILC consist of nine-cell cavities based on the TESLA design. In order to facilitate reaching higher gradients we have re-designed the cavity shape. This leads to a reduction, comparable to several current designs, in both the ratio of the surface electric field to the accelerating field (Es/Ea) and the magnetic field to the accelerating field (Bs/Ea). The bandwidth of the accelerating mode is also optimized. This new shape, which we refer to as the New Low Surface Field (NLSF) design, bears comparison with the Ichiro, Re-entrant and LSF designs.

 
TH5PFP052 Electron Cloud Simulations for ANKA electron, simulation, vacuum, undulator 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.

 
TH5PFP057 Measured and Calculated Field Properties of the SIS 100 Magnets Described Using Elliptic and Toroidal Multipoles multipole, synchrotron, antiproton, vacuum 3336
 
  • E.S. Fischer, A. Mierau, P. Schnizer
    GSI, Darmstadt
  • P.G. Akishin
    JINR, Dubna, Moscow Region
  • R.V. Kurnyshov
    Electroplant, Moscow
  • B. Schnizer
    TUG/ITP, Graz
  • P.A. Shcherbakov
    IHEP Protvino, Protvino, Moscow Region
 
 

The first full size superconducting dipole magnets for the SIS 100 Tm synchrotron were built and tested. The achieved magnetic field has been measured with a rotating coil probe. An intensive Finite Element R&D, necessitated by the used superconducting cable as well as by the complex mechanical coil and yoke structure, allows calculating the field with high accuracy. Elliptic multipoles were used to describe the field within the whole aperture of the vacuum chamber. As the final design for the SIS 100 dipoles is curved, we developed toroidal multipoles describing the field within a curved magnet, and enabling us to interpret the measurement of a rotating coil probe within such magnets. We describe the performance of the magnetic measurement system, present the measured field properties and compare them to the calculated ones.

 
TH5PFP059 Numerical Calculation of Wake Fields in Structures with Conductive Walls vacuum, wakefield, multipole, electromagnetic-fields 3342
 
  • A.V. Tsakanian
    Uni HH, Hamburg
  • M. Dohlus, I. Zagorodnov
    DESY, Hamburg
 
 

Based on TE/TM splitting algorithm a new (longitudinally) dispersion-free numerical scheme is developed to evaluate the wake fields in structures with finite wall conductivity. The impedance boundary condition in this scheme is modeled by the one dimensional wire connected to boundary cells. A good agreement of the numerical simulations with the analytical results is obtained. The developed code allows to calculate multipole wake potentials of arbitrary shaped geometries with walls of finite high conductivity.

 
TH5PFP079 Statistical Analysis of Multipole Components in the Magnetic Field of the RHIC Arc Regions quadrupole, multipole, sextupole, interaction-region 3386
 
  • J. Beebe-Wang, A.K. Jain
    BNL, Upton, Long Island, New York
 
 

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


The existence of multipolar components in the dipole and quadrupole magnets is one of the factors limiting the beam stability in the RHIC operations. Therefore, the statistical properties of the non-linear fields are crucial for understanding the beam behavior and for achieving the superior performance in RHIC. In an earlier work*, the field quality analysis of the RHIC interaction regions (IR) was presented. Furthermore, a procedure for developing non-linear IR models constructed from measured multipolar data of RHIC IR magnets was described. However, the field quality in the regions outside of the RHIC IR regions had not yet been addressed. In this paper, we present the statistical analysis of multipolar components in the magnetic fields of the RHIC arc regions. The emphasis is on the lower order components, especially the sextupole in the arc dipole and the 12-pole in the quadrupole magnets, since they are shown to have the strongest effects on the beam stability. Finally, the inclusion of the measured multipolar components data of RHIC arc regions and their statistical properties into tracking models is discussed.


*J. Beebe-Wang and A. Jain, “Realistic Non-linear Model and Field Quality Analysis in RHIC Interaction Regions”, proc. of PAC 2007, page 4309-4311 (2007)

 
TH5RFP024 Instrumentation for High Frequency Cavity BPM in CALIFES cavity, linac, single-bunch, controls 3497
 
  • C.S. Simon, D. Bogard, M. Luong
    CEA, Gif-sur-Yvette
 
 

The probe beam linac of the CTF3 test facility, named CALIFES, is developed by the CEA Saclay, the LAL Orsay and CERN to deliver short bunches (0.75 ps) with a charge of 0.6 nC to the CLIC 12 GHz accelerating structures. To setup the machine and obtain a precise beam handling, six high resolution beam position monitors (BPMs), based on a radiofrequency reentrant cavity with an aperture of 18 mm, are installed along the linac. The associated electronics is composed of an analog signal processing electronics with a multiplexing to control the six monitors. Due to mechanical tolerances, dipole mode frequencies are different for each BPMs, 100 MHz IF frequency is, therefore, used so that monitors operate in single and multi-bunches. Digitalised signals from acquisition boards are made available to the operation crew thanks to the OASIS interfaces. In this paper, the BPMs acquisition and the signal post processing, to extract the beam position, will be discussed and first beam tests will be presented.

 
TH5RFP025 Beam Measurements at the ALBA Linac linac, emittance, quadrupole, diagnostics 3500
 
  • U. Iriso, G. Benedetti, A. Olmos
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The ALBA Linac is a turn-key system able to produce 4 nC electron beams at 100 MeV beams with a normalized emittance below 30 mm*mrad. Beam position stability below 0.1 mm is measured using new BPM electronics. Thorough analysis are carried out to measure the beam emittance, energy and energy spread. This paper discusses the measurement techniques, analysis method, and results obtained during the Linac commissioning.

 
TH5RFP038 Longitudinal Schottky Spectrum of the Peak Bunch Amplitude Signal synchrotron, quadrupole, diagnostics, pick-up 3531
 
  • E.N. Shaposhnikova, T. Bohl, T.P.R. Linnecar
    CERN, Geneva
 
 

Diagnostic techniques based on the Schottky spectrum of the peak detected signal have been used at CERN for a long time to study the behaviour of bunched beams. In this paper it is shown how the measured spectrum is related to the particle distribution in synchrotron frequency. The experimental set-up used and its limitations are also presented together with examples of beam measurements in the SPS and LHC.

 
TH5RFP040 Resonant-Cavity Diagnostics for an Emittance Exchange Experiment cavity, coupling, emittance, quadrupole 3537
 
  • N. Barov, J.S. Kim, D.J. Newsham
    Far-Tech, Inc., San Diego, California
 
 

The emittance exchange experiment planned at the Argonne Wakefiel Accelerator facility will rely on a set of cavity-based beam diagnostics in order to map the transport matrix through the beamline. These will include cavity BPM and time-of-flight diagnostics, as well as quadrupole cavity x-y coupling diagnostics. The measurement system will be designed to fit within compact space requirements, while also maintaining a sufficient clear aperture and sensitivity. The RF design of the system, as well as RF cold-test data for the BPM cavities, is presented.

 
TH5RFP051 A Laser-Based Beam Profile Measuring Instrument for the Front End Test Stand at RAL ion, laser, electron, ion-source 3567
 
  • D.A. Lee, P. Savage
    Imperial College of Science and Technology, Department of Physics, London
  • C. Gabor
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • J.K. Pozimski
    STFC/RAL, Chilton, Didcot, Oxon
 
 

The RAL Front End Test Stand is being constructed to demonstrate production of a high-quality, chopped 60 mA H- beam at 3 MeV and 50 pps. In parallel to the accelerator development, non-destructive laser-based beam diagnostics are being designed. This paper reports on the realisation of a laser-based profile instrument that will be able to reconstruct the complete 2D transverse beam density distribution by scanning a laser beam through the ion beam at a variety of angles and then computationally combining the results. Commissioning results are presented alongside plans for future developments.

 
TH5RFP052 Fermilab HINS Proton Ion Source Beam Measurements solenoid, proton, emittance, linac 3570
 
  • W.M. Tam
    IUCF, Bloomington, Indiana
  • G. Apollinari, S. Chaurize, S. Hays, G.V. Romanov, V.E. Scarpine, C.W. Schmidt, W.M. Tam, R.C. Webber
    Fermilab, Batavia
 
 

The proton ion source for the High Intensity Neutrino Source (HINS) Linac front-end at Fermilab has been successfully commissioned. It produces a 50 keV, 3 msec beam pulse with a peak current greater than 20 mA at 2.5 Hz. The beam is transported to the radio-frequency quadrupole (RFQ) by a low energy beam transport (LEBT) that consists of two focusing solenoids, four steering dipole magnets and a beam current transformer. To understand beam transmission through the RFQ, it is important to characterize the 50 keV beam before connecting the LEBT to the RFQ. A wire scanner and a Faraday cup are temporarily installed at the exit of the LEBT to study the beam parameters. Beam profile measurements are made for different LEBT settings and results are compared to those from computer simulations. In lieu of direct emittance measurements, a solenoid variation method based on profile measurements is used to reconstruct the beam emittance.

 
TH5RFP057 Fast Horizontal e+ Instability Measurements in DAΦNE positron, feedback, electron, simulation 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.

 
TH5RFP085 Tunnel and Magnet Survey of KEKB after Ten Years of Operation survey, quadrupole, alignment, sextupole 3648
 
  • M. Masuzawa, Y. Ohsawa, N. Ohuchi
    KEK, Ibaraki
 
 

KEKB is a double-ring collider with a circumference of 3016 m. The two rings were built side-by-side in the TRISTAN tunnel, 11 m below ground. KEKB has been operating successfully for about 10 years, since 1999, and its peak luminosity continues to improve. During the summer shutdown of 2008, the magnet tilts were measured for the first time since installation and it was found that some magnets were rotated over time. The tunnel level marker and the magnet height were also surveyed. The south region of the tunnel is sinking, resulting in magnet level changes. The survey results will be reported in this paper.

 
TH6PFP016 Numerical Based Linear Model for Dipole Magnets optics, focusing, lattice, quadrupole 3732
 
  • Y. Li, S. Krinsky, M. Rehak
    BNL, Upton, Long Island, New York
 
 

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


In this paper, we discuss an algorithm for constructing a numerical linear optics model for dipole magnets from a 3D field map. The difference between the numerical model and K. Brown’s analytic approach is investigated and clarified. It was found that the optics distortion due to the dipoles’ fringe focusing must be properly taken into account to accurately determine the chromaticities. In NSLS-II, there are normal dipoles with 35-mm gap and dipoles for infrared sources with 90-mm gap. This linear model of the dipole magnets is applied to the NSLS-II lattice design to match optics parameters between the DBA cells having dipoles with different gaps.

 
TH6PFP027 ALBA Booster Settings for an Optimized Performance sextupole, quadrupole, dynamic-aperture, lattice 3756
 
  • G. Benedetti, D. Einfeld, J. Marcos, M. Muñoz, M. Pont
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The ALBA booster is a 100 MeV-3 GeV ramping synchrotron, with large circumference of 249.6 m and low emittance of 9nm*rad, cycling at 3 Hz. The lattice consists of a 4-fold symmetric modified FODO lattice with defocusing gradient dipoles. Magnetic measurements on all magnets have been performed: the studies and lattice settings to recover the design optics preserving good machine performances, such as the lattice flexibility, the low beta functions and large dynamic aperture at high chromaticities, are presented.

 
TH6PFP028 Model Independent Analysis with Coupled Beam Motion coupling, betatron, resonance, simulation 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)

 
TH6PFP029 Bunch Compression for a Short-Pulse Mode in Cornell's ERL linac, quadrupole, emittance, acceleration 3762
 
  • J.R. Thompson, G.H. Hoffstaetter
    CLASSE, Ithaca, New York
 
 

The production of ultra-short x-rays in Cornell's Energy Recovery Linac (ERL) requires electron bunch lengths of less than 100fs with minimal transverse emittance growth and energy spread. Because the linac consists of two sections separated by an arc, CSR forces limit the bunch length in the linac, and bunch compression has to be installed after acceleration. Creation of such short bunches requires a second order bunch compression scheme with correction of the third order dispersion. In this paper, we discuss possible bunch compression systems and explore the benefits of each using the tracking program TAO including CSR forces. Overall, we find that a FODO compressor utilizing dipole, quadrupole and sextupole magnets can achieve the design goals of the short pulse mode.

 
TH6PFP043 Orbit, Optics and Chromaticity Correction for PS2 Negative Momentum Compaction Lattices sextupole, quadrupole, resonance, optics 3802
 
  • Y. Papaphilippou, J. Barranco, W. Bartmann, M. Benedikt, C. Carli
    CERN, Geneva
  • R. De Maria, S. Peggs, D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

The effect of magnet misalignments in the beam orbit and linear optics functions are reviewed and correction schemes are applied to the negative momentum compaction lattices of PS2. Chromaticity correction schemes are also proposed and tested with respect to off-momentum optics properties. The impact of the correction schemes in the dynamic aperture of the different lattices is finally evaluated.

 
TH6PFP044 Linear Optics Design of Negative Momentum Compaction Lattices for PS2 optics, injection, quadrupole, resonance 3805
 
  • Y. Papaphilippou, J. Barranco, W. Bartmann, M. Benedikt, C. Carli, B. Goddard
    CERN, Geneva
  • R. De Maria, S. Peggs, D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

In view of the CERN Proton Synchrotron proposed replacement with a new ring (PS2), a detailed optics design as been undertaken following the evaluation of several lattice options. The basic arc module consists of cells providing negative momentum compaction. The straight section is formed with a combination of FODO and quadrupole triplet cells, to accommodate the injection and extraction systems, in particular the H- injection elements. The arc is matched to the straight section with a dispersion suppressor and matching module. Different lattices are compared with respect to their linear optics functions, tuning flexibility and geometrical acceptance properties.

 
TH6PFP051 Muon Collider Lattice with Local Interaction Region Chromaticity Correction sextupole, collider, lattice, quadrupole 3820
 
  • Y. Alexahin, E. Gianfelice-Wendt
    Fermilab, Batavia
 
 

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


Muon collider is a promising candidate for the next energy frontier machine. In order to obtain peak luminosity of the order of 1035/cm2/s in the TeV energy range the beta function at the interaction point should be smaller than 1cm. To obtain correspondingly small bunch length with a reasonable RF voltage (within 1GV) the momentum compaction factor should be smaller than 10-4 in the momentum range ~1%. The lattice design must also provide sufficient dynamic aperture for ~20 microns normalized beam emittance and minimum possible circumference. Together these requirements present a challenge which has never been met before. We offer a solution to this problem which has the following distinctive features: i) chromatic compensation achieved with sextupoles and dispersion generating dipoles placed near the IR quadrupoles (not in a special section), ii) low value of momentum compaction factor obtained by balancing positive contribution from the arcs with negative contribution from the suppressors of the generated in the IR dispersion. Theoretical aspects and various options will be discussed.

 
TH6PFP052 A Simple Transition-Free Lattice of an 8 GeV Proton Synchrotron lattice, sextupole, synchrotron, proton 3823
 
  • W. Chou
    Fermilab, Batavia
 
 

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


A transition-free lattice is a basic requirement of a high-intensity medium-energy (several GeV) proton synchrotron in order to eliminate beam losses during transition crossing. An 8 GeV synchrotron is proposed as a principal component in an alternative hybrid design of Project-X. This machine would be housed in the Fermilab antiproton source enclosure replacing the present Debuncher. A simple doublet lattice with high transition gamma has been designed. It uses just one type of dipoles and one type of quadrupoles (QF and QD are of the same length). It has no transition crossing. It has a triangular shape with three zero dispersion straight sections, which can be used for injection, extraction, RF and collimators. The beta-functions and dispersion are low. This lattice has plenty of free space for correctors and diagnostic devices, as well as good optical properties including large dynamic aperture, weak dependence of lattice functions on amplitude and momentum deviation.


*W. Chou, “An Alternative Approach to Project X,” this conference.

 
TH6PFP058 Linear Optics Measurement and Correction in the SNS Accumulator coupling, quadrupole, optics, betatron 3838
 
  • Z. Liu
    IUCF, Bloomington, Indiana
  • S.M. Cousineau, J.A. Holmes, M.A. Plum
    ORNL, Oak Ridge, Tennessee
 
 

Funding: Division of Materials Science, U.S. Department of Energy, under contract number DE-AC05-96OR22464 with UT-Battelle Corporation for Oak Ridge National Laboratory


In order to achieve a more robust and optimal performance, the difference between the real machine and its underlying model should be understood and eliminated. Discrepancies between the measuremed and predicted linear optics suggest possible errors of the focusing magnets and diagnostic devices. To find and correct those errors, a widely used method, orbit response matrix (ORM)* approach is applied to the SNS storage ring, which successfully brings the tune deviation from 3% to 0.1%, improves horizontal beta beating from 15% to 3%, and perfectly flattens the orbit. In this article, we discussed the progress and possible future improvements with the SNS ring optics correction.


*J. Safranek, "Experimental determination of storage ring optics using closed orbit response measurements", Nucl. Inst. and Meth. A388, (1997), pg. 27

 
TH6PFP066 The Correction of Linear Lattice Gradient Errors Using an AC Dipole quadrupole, simulation, betatron, optics 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.

 
TH6REP016 Analysis of Contribution from Edge Radiation to Optical Diffraction Radiation radiation, electron, synchrotron, synchrotron-radiation 3984
 
  • C. Liu
    PKU/IHIP, Beijing
  • P. Evtushenko, A. Freyberger, C. Liu
    JLAB, Newport News, Virginia
  • A.H. Lumpkin
    Fermilab, Batavia
 
 

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


Beam size measurement with near-field optical diffraction radiation (ODR) has been carried out successfully at CEBAF. The ODR station is installed on the Hall-A beam line after eight bending magnets. The ODR images were affected by an unexpected radiation. Some calculations for analyzing the source of the radiation will be presented. Furthermore, two schemes will be proposed to alleviate the contamination.

 
TH6REP024 A Proposal of a Single Coupler Cavity Beam Position Monitor cavity, coupling, simulation, 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.

 
TH6REP025 Development of the S-Band BPM System for ATF2 cavity, extraction, coupling, target 4003
 
  • A. Lyapin, B. Maiheu, M. Wing
    UCL, London
  • R. Ainsworth, A.S. Aryshev, S.T. Boogert, G.E. Boorman, S. Molloy
    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
  • 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 this goal is the high resolution cavity beam position monitors (BPMs). In this paper we report on the S-band system installed in the final focus region of the new ATF2 extraction beamline. It only includes 4 BPMs, but they are mounted on the most critical final focus magnets squeezing the beam down to 35 nm. We discuss both the design and the first operational experience with the system.

 
TH6REP035 Beam Diagnostic by Outside Beam Chamber Fields impedance, pick-up, coupling, diagnostics 4024
 
  • A. Novokhatski, S.A. Heifets
    SLAC, Menlo Park, California
  • A.V. Aleksandrov
    ORNL, Oak Ridge, Tennessee
 
 

Funding: work supported by the Department of Energy under contract number DE-AC03-76SF00515 and DE-AC05


Fields induced by a beam and penetrated outside the beam pipe can be used for a beam diagnostic. Wires placed in longitudinal slots in the outside wall of the beam pipe can work as a beam pickup. This has a very small beam-coupling impedance and avoids complications of having a feed-through. The signal can be reasonably high at low frequencies. We calculate the beam-coupling impedance due to a long longitudinal slot in the resistive wall and the signal induced in a wire placed in such a slot and shielded by a thin screen from the beam. We present a field waveform at the outer side of a beam pipe, obtained as a result of calculations and measurements. Such kind of diagnostic can be used in storage rings, synchrotron light sources, and free electron lasers, like LINAC coherent light source.

 
FR5PFP008 A Statistical Study of Beam Centroid Oscillations in a Solenoid Transport Channel solenoid, lattice, alignment, focusing 4323
 
  • S.M. Lund, J.E. Coleman, S.M. Lidia, P.A. Seidl, C.J. Wootton
    LBNL, Berkeley, California
 
 

Funding: This research was performed under the auspices of the U.S. DOE at the Lawrence Livermore and Lawrence Berkeley National Laboratories under Contracts No. DE-AC52-07NA27344 and No. DE-AC02-05CH11231.


A recent theory in Ref. * analyzes small-amplitude oscillations of the transverse beam centroid (center of mass) in solenoidal transport channels. This theory employs a transformation to a rotating Larmor frame to simply express the centroid response to mechanical misalignments (transverse center displacements and tilts about the of the longitudinal axis of symmetry) of the solenoid and initial centroid errors. The centroid evolution is expressed in terms of a superposition of the centroid evolving in the ideal aligned system plus an expansion in terms of "alignment functions" that are functions of only the ideal lattice with corresponding amplitudes set by the solenoid misalignment parameters. This formulation is applied to analyze statistical properties of beam centroid oscillations induced by solenoid misalignments. Results are compared to experiments at the NDCX experiment at the LBNL. It is found that contributions to oscillation amplitudes from tilts are significantly larger than contributions from offsets for expected parameters. Use of the formulation to optimally steer the centroid back on-axis with limited diagnostic measurements is also discussed.


* S.M. Lund, C.J. Wootton, and E.P. Lee, "Transverse centroid oscillations in solenoidally focused beam transport lattices," accepted for publication, Nuc. Inst. Meth. A.

 
FR5PFP012 Orbit Response Matrix Measurements in the Los Alamos Proton Storage Ring quadrupole, storage-ring, closed-orbit, coupling 4332
 
  • J.S. Kolski, R.J. Macek, R.C. McCrady
    LANL, Los Alamos, New Mexico
  • J.S. Kolski
    IUCF, Bloomington, Indiana
 
 

Funding: US DOE #DE-AC52-06NA25396


Orbit response matrix techniques have been used in numerous electron storage rings to elucidate various optical properties of the machines. Such measurements in a long-pulse accumulator ring have unique complications. We present here the techniques and results of such a measurement at the Los Alamos Proton Storage Ring*. We also show the deficiencies in previous models of the ring and a comparison of the beta-functions as fit by the orbit response method to direct measurements by quadrupole magnet variations.


*LA-UR- 08-07694

 
FR5PFP022 Proton Storage Ring Optics Modeling with ac-Driven Betatron Motion betatron, storage-ring, optics, proton 4356
 
  • Y.T. Yan, A. Chao
    SLAC, Menlo Park, California
  • M. Bai
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE


Unlike an electron storage ring with radiation damping, resonance excitation is unsuitable to a proton storage ring for turn-by-turn betatron orbit data. However, one may consider modified betatron motion driven by ac dipoles oscillating at frequencies near the betatron tunes. With a matrix formulation for adding ac-dipole effects on 2-D coupled one-turn map, we concatenate the ac-dipole effects and the one-turn map to obtain a modified linear map. The ac-dipole effects are equivalent to inserted symplectic linear maps at the ac-dipole locations. If the maps are normalized through decoupling similarity transformation, the decoupled maps for the ac-dipole effects are equivalent to 1-D thin quads inserted at the corresponding locations, the same conclusion for the 1-D driven oscillation*. For optics modeling with MIA technique**, one must make sure that there are, simultaneously, two transverse ac-dipole driven betatron oscillations along with one longitudinal synchrotron oscillation. Once the optics model for the modified betatron motion is obtained, one can then obtain the proton storage ring model by de-concatenating the inserted ac-dipole linear maps.


* R. Miyamoto, S.E. Kopp, A. Jansson, and M.J. Syphers, PRSTAB 11, 084002 (2008).
** Y.T. Yan, ICFA Beam Dynamics Newsletter, No. 42, pp. 71-87 ( 2007), Y. Cai, W. Chou, Eds.

 
FR5PFP036 Closed Orbit Correction of Hefei Advanced Light Source (HALS) Storage Ring closed-orbit, sextupole, quadrupole, storage-ring 4384
 
  • G. Feng, W. Li, L. Liu, L. Wang, C.-F. Wu, H. Xu, S.C. Zhang
    USTC/NSRL, Hefei, Anhui
 
 

In order to meet the increasing requirements of synchrotron radiation users, a new plan of VUV and soft X-ray light source, named Hefei Advanced Light Source (HALS), is brought forward by National Synchrotron Radiation Laboratory (NSRL). This 1.5GeV storage ring with ultra low emittance 0.2nmrad consists of 18 combined FBA cells and the circumference is 388m. Strong enough quadrupoles and sextupoles must be needed for getting such low emittance lattice, which will lead beam close orbit distortions’ (COD) sensitivity to the field and alignment errors in magnets. Estimation of the COD from various error sources is investigated. Using orbit response matrix and singular value decomposition method, the distribution of beam position monitors and the location of correctors are reported in the paper. Simulation proves that COD can be corrected down to 60 microns level. In the same time the corrector strengths are weaker enough in the correction scheme.

 
FR5PFP056 Beam Dynamics and RF Cavity Design of a Standing/Traveling-Wave Hybrid Photoinjector for High Brightness Beam Generation gun, quadrupole, cavity, linac 4434
 
  • A. Fukasawa, H. Badakov, B.D. O'Shea, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • D. Alesini, L. Ficcadenti, B. Spataro
    INFN/LNF, Frascati (Roma)
  • L. Palumbo
    Rome University La Sapienza, Roma
 
 

A hybrid photoinjector, which we present here, consists of a 6-cell traveling wave structure with a standard 1.6-cell RF gun attached to the one end and a 3-m long linac following for further acceleration. With this structure, no reflection observed at the input port. This enables to build the accelerator without a circulator which limits the power and the frequency of RF. From the beam dynamics point of view, the beam is produced as the normal RF guns and gets short by velocity bunching in the traveling wave section right after the gun. The peak current can reach more than 1 kA, with about 2 mm.mrad of the emittance at 20 MeV. We discuss more details about the beam dynamics as well as the RF structure.

 
FR5PFP089 Modeling Microwave Transmission in Electron Clouds electron, resonance, simulation, plasma 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 simulation, quadrupole, 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.

 
FR5RFP021 Acceleration of an Electron Bunch with Narrow Energy Spread in a PWFA plasma, wakefield, electron, resonance 4576
 
  • P. Muggli
    UCLA, Los Angeles, California
  • B.A. Allen
    USC, Los Angeles, California
  • M. Babzien, K. Kusche, J.H. Park, V. Yakimenko
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by US Department of Energy.


One of the challenges for plasma wakefield accelerators (PWFAs) is to accelerate a trailing bunch with a narrow energy spread. The real challenge is to produce a bunch train with a least one drive bunch and one trailing bunch. We have demonstrated experimentally at the BNL-ATF a mask technique that can produce trains of bunches with variable spacing in the sub-picosecond range*. This 60 MeV train with one to five drive bunches and a trailing bunch propagates in a 1 to 2 cm long plasma capillary discharge with a variable plasma density. When the plasma density is tuned such that the plasma wavelength is equal to the drive bunches spacing the plasma wakefield is resonantly excited. The distance between the last drive bunch and the trailing bunch is one and a half time that between the drive bunches, putting the trailing bunch in the accelerating phase of the wakefield. The resonance is characterized by a maximum energy loss by all the drive bunches and maximum energy gain by the trailing bunch. Experimental results will be presented.


*P. Muggli et al., Phys. Rev. Lett. {10}1, 054801, 2008

 
FR5RFP032 Infrared Extraction Chamber for the NSLS-II Storage Ring extraction, impedance, radiation, electron 4598
 
  • A. Blednykh, G.L. Carr, D.S. Coburn, S. Krinsky
    BNL, Upton, Long Island, New York
 
 

The short- and long-range wakepotentials have been studied for the design of the infrared (IR) extraction chamber with large full aperture: 67mm vertical and 134mm horizontal. The IR-chamber will be installed within a 2.6m long wide-gap bending magnet with 25m bend radius. Due to the large bend radius it is difficult to separate the light from the electron trajectory. The required parameters of the collected IR radiation in location of the extraction mirror are ~50mrad horizontal and ~25mrad vertical (full radiation opening angles). If the extraction mirror is seen by the beam, resonant modes are generated in the chamber. In this paper, we present the detailed calculated impedance for the design of the far-IR chamber, and show that placing the extraction mirror in the proper position eliminates the resonances. In this case, the impedance reduces to that of a simple tapered structure, which is acceptable in regard to its impact on the electron beam.

 
FR5RFP043 Simulations of Electron-Cloud Current Density Measurements in Dipoles, Drifts and Wigglers at CesrTA simulation, wiggler, electron, 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, positron, simulation, 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.

 
FR5RFP061 Stability of Flat Bunches in the Recycler Barrier Bucket proton, space-charge, damping, electron 4679
 
  • T. Sen, C.M. Bhat, J.-F. Ostiguy
    Fermilab, Batavia
 
 

We examine the stability of intense flat bunches in barrier buckets. We consider a class of stationary distributions and derive analytical expressions for the threshold intensity at which Landau damping is lost against rigid dipole oscillations in the presence of impedances and space charge forces. Particle simulations are used to follow the dynamics in a barrier bucket and compare with the analytic expressions. These studies are related to experimental observations in the Recycler ring at Fermilab.

 
FR5RFP071 Maps for Electron Clouds: Application to LHC Conditioning electron, simulation, vacuum, 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).

 
FR5RFP075 Transverse Periodic Beam Loading Effects in a Storage Ring cavity, storage-ring, emittance, beam-loading 4710
 
  • J.R. Thompson, J.M. Byrd
    LBNL, Berkeley, California
 
 

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


Uneven beam fill patterns in storage rings, such as gaps in the fill patterns, leads to periodic, or transient loading of the modes of the RF cavities. We show that an analogous effect can occur in the loading of a dipole cavity mode when the beam passes off the electrical center of the cavity mode. Although this effect is small, it results in a variation of the transverse offset of the beam along the bunch train. For ultralow emittance beams, such as optimized third generation light sources and damping rings, this effect results in a larger projected emittance of the beam compared with the single bunch emittance. The effect is particularly strong for the case when a strong dipole mode has been purposely added to the ring, such as a deflecting, or ‘‘crab'' cavity. We derive an approximate analytic solution for the variation of the beam-induced deflecting voltage along the bunch train. We also show via a tracking simulation the combined effect of the periodic loading of the fundamental and dipole modes.

 
FR5RFP076 Initial Results of Simulation of a Damping System for Electron Cloud-Driven Instabilities in the CERN SPS feedback, electron, simulation, 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.

 
FR5RFP078 Update on Electron-Cloud Simulations Using the Package WARP-POSINST electron, simulation, lattice, emittance 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.

 
FR5RFP087 The Effect of an Oxide Layer on Resistive-Wall Wake Fields wakefield, FEL, electron, damping 4743
 
  • A. Novokhatski
    SLAC, Menlo Park, California
 
 

Funding: work supported by the Department of Energy under contract number DE-AC03-76SF00515


Shorter and shorter electron bunches are now used in the FEL designs. The fine structure of the wall of a beam vacuum pipe plays more noticeable role in the wake field generation. Additionally to the resistance and roughness, the wall may have an oxide layer, which is usually a dielectric. It is important for aluminum pipe, which have Al2O3 layer. The thickness of this layer may vary in a large range: 1-100 nm. We study this effect for the very short (20-1000 nm) ultra relativistic bunches in an infinite round pipe. We solved numerically the Maxwell equations for the fields in the metal and ceramics. Results showed that the oxide layer may considerably increase the wavelength and the decay time of the resistive-wall wake fields, however the loss factor of the very short bunches does not change much.

 
FR5REP029 A Novel Beam Steering Algorithm with Orbit Response Matrix closed-orbit, controls, injection, space-charge 4829
 
  • C. Wu, E.H. Abed, B.L. Beaudoin, S. Bernal, K. Fiuza, 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.


Beam centroid control is an important method for optimizing the performance for accelerators, including the University of Maryland Electron Ring (UMER), which is a scaled low-energy (10KeV) storage ring. The conventional response matrix and singular value decomposition approach do not work well on the UMER because of the unique ring structure. One of the purposes of this work is to verify that the beam centroid could be controlled in the presence of very strong space charge. In this paper, we present a novel algorithm which is based on the singular value decomposition, but uses a different response matrix, which is computed from the closed equilibrium orbit and beam positions up to the first four turns in the multi-turn beam circulation. Other issues like strong coupling between the horizontal steering dipoles and vertical steering dipoles in the beam injection section will be addressed. Implementation of this algorithm leads to significant improvement on the beam positions and multi-turn operation.

 
FR5REP094 Tracking Periodic Parameters in the Measured Magnetic Field Maps of a Spiral FFAG closed-orbit, lattice, extraction, injection 4999
 
  • F. Méot
    CEA, Gif-sur-Yvette
  • F. Forest, M.J. Leray
    Sigmaphi, Vannes
  • J. Pasternak
    Imperial College of Science and Technology, Department of Physics, London
 
 

Funding: Agence Nationale de la Recherche, France, contract NT05-1_41853


A prototype of a spiral lattice FFAG magnet has been constructed in the frame of the RACCAM project*. THis magnet is subject to extensive field measurements and 3-dimensional field map measurements. The properties and qualities of the magnet are assessed directly from ray-tracing, using stepwise integration, for deriving lattice parameters as tunes, chromaticities, dynamic paertures, etc. Reporting on this is the subject of the poster.


*http://lpsc.in2p3.fr/service_accelerateurs/raccam.htm

 
FR5REP108 EMMA Diagnostic Line injection, extraction, diagnostics, septum 5026
 
  • B.D. Muratori, J.K. Jones, S.L. Smith, S.I. Tzenov
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

EMMA (Electron Machine with Many Applications) is a prototype non-scaling electron FFAG to be hosted at Daresbury Laboratory. NS-FFAGs related to EMMA have an unprecedented potential for medical accelerators for carbon and proton hadron therapy. It also represents a possible active element for an ADSR (Accelerator Driven Sub-critical Reactor). This paper will summarize the design of the extraction / diagnostic transfer line of the NS-FFAG. In order to operate EMMA, the energy recovery linac ALICE shall be used as injector and the energy will range from 10 to 20 MeV. Because this would be the first non-scaling FFAG, it is important that as many of the bunch properties are studied as feasible, both at injection and at extraction. To do this, a complete diagnostic line was designed consisting of a tomography module together with several other diagnostic devices including the possibility of using a transverse deflecting cavity. Details of the diagnostics are also presented.

 
FR5REP110 Magnetic Measurements of the RACCAM Prototype FFAG Dipole alignment, instrumentation, simulation, 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.

 
FR5REP118 An Alternative Ion-Optical Mode of the Recuperated Experimental Storage Ring (RESR) dynamic-aperture, sextupole, ion, quadrupole 5056
 
  • S.A. Litvinov, A. Dolinskyy, O.E. Gorda, F. Nolden, M. Steck
    GSI, Darmstadt
 
 

The main purpose of the Recuperated Experimental Storage Ring (RESR) in the FAIR project is the accumulation of antiprotons coming from the Collector Ring (CR), where they are stochastically pre-cooled. The accumulation scheme in the RESR foresees longitudinal stacking in combination with stochastic cooling. The stochastic cooling process strongly depends on the slip factor η of the ring. Presently, the RESR is designed to operate with small slip factor of 0.03. In order to increase the flexibility for optimized stochastic cooling a new alternative ion-optical mode with higher slip factor of 0.11 has been calculated in such a way, that the RESR can be operated with a fixed magnetic structure in both modes. The influence of the high-order chromaticity on the particle motion has been investigated and a chromaticity correction scheme is applied. The variation of the transition energy over the momentum acceptance was examined and the possibility of its correction is described.