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lattice

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MOZMH01 Experience and Lessons with the SNS Superconducting Linac cavity, linac, beam-losses, emittance 26
 
  • Y. Zhang
    ORNL, Oak Ridge, Tennessee
 
 

Experience and lessons with the SNS superconducting linac over the first 5 years of commissioning and operation are reviewed. As the beam power was ramped up to 1 MW, the linac beam loss has been maintained below 1 W/m and residual activation has been held to a safe level. This can be attributed mainly to a robust accelerator design as well as to dedicated beam dynamics studies during this period. In addition to a review of both transverse and longitudinal beam phase-space measurements, we will review several hardware lessons learned with this high-power proton linac − such as nonlinear multipole components of the linac quadrupoles, beam collimators, high-order-mode couplers of the superconducting cavities, and cavity piezo tuners.

 

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MOOCMH01 Accelerator Physics Issues for the TPS coupling, emittance, booster, multipole 36
 
  • C.-C. Kuo, H.-P. Chang, H.C. Chao, M.-S. Chiu, P.J. Chou, G.-H. Luo, A. Rusanov, H.-J. Tsai, F.H. Tseng, C.H. Yang
    NSRRC, Hsinchu
 
 

Taiwan Photon Source (TPS) is a low emittance third-generation light source which is currently under construction in the NSRRC site in Taiwan. TPS consists of 24 double-bend cells and its circumference is 518.4 m. A 496.8-m booster with multi-bend structure is designed. The alternative lattices, such as high/low betax, chicanes with double-vertical-waists in the long straights, and short bunches with low momentum compactions, etc., are investigated. Orbit and coupling corrections and stability issues are studied. Touschek lifetime and effects due to insertion devices are simulated. Works on impedance estimation and instability simulations are performed.

 

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MOPEA021 PAMELA Overview and Status proton, extraction, injection, multipole 112
 
  • K.J. Peach, J.H. Cobb, S.L. Sheehy, H. Witte, T. Yokoi
    JAI, Oxford
  • M. Aslaninejad, M.J. Easton, J. Pasternak
    Imperial College of Science and Technology, Department of Physics, London
  • R.J. Barlow, H.L. Owen, S.C. Tygier
    UMAN, Manchester
  • C.D. Beard, P.A. McIntosh, S.M. Pattalwar, S.L. Smith, S.I. Tzenov
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • N. Bliss, T.J. Jones, J. Strachan
    STFC/DL, Daresbury, Warrington, Cheshire
  • T.R. Edgecock, J.K. Pozimski
    STFC/RAL, Chilton, Didcot, Oxon
  • R.J.L. Fenning, A. Khan
    Brunel University, Middlesex
  • I.S.K. Gardner, D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • M.A. Hill
    GIROB, Oxford
  • C. Johnstone
    Fermilab, Batavia
  • B. Jones, B. Vojnovic
    Gray Institute for Radiation Oncology and Biology, Oxford
  • R. Seviour
    Cockcroft Institute, Lancaster University, Lancaster
 
 

The status of PAMELA (Particle Accelerator for MEdicaL Applications) ' an accelerator for proton and light ion therapy using a non-scaling FFAG (ns-FFAG) accelerator ' is reviewed and discussed.

 
MOPEA022 PAMELA: Lattice Solution for a Medical C6+ Therapy Facility proton, multipole, resonance, octupole 115
 
  • S.L. Sheehy, K.J. Peach, H. Witte, T. Yokoi
    JAI, Oxford
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

PAMELA (Particle Accelerator for MEdicaL Applications) employs novel non-scaling Fixed Field Alternating Gradient (NS-FFAG) technology in the development of a proton and C6+ particle therapy facility. One of the challenges of this design is the acceleration of high energy C6+ in a lattice which enables high flexibility and reliability for treatments, yet remains minimal in size and complexity. Discussed here is the Carbon 6+ lattice solution in terms of both design and performance.

 
MOPEA028 Lattice Design for the ERL Electron Ion Collider in RHIC electron, ion, linac, collider 127
 
  • D. Trbojevic, J. Beebe-Wang, X. Chang, Y. Hao, A. Kayran, V. Litvinenko, B. Parker, V. Ptitsyn, N. Tsoupas
    BNL, Upton, Long Island, New York
  • E. Pozdeyev
    FRIB, East Lansing, Michigan
 
 

We present a medium-energy (4 GeV) electron ion collider (MeRHIC) lattice design for the Relativistic Heavy Ion Collider (RHIC). MeRHIC represents a staged approach towards the higher energy eRHIC, with MeRHIC hardware being reused for eRHIC. The lattice design includes two Energy Recovery Linacs (ERLs), multiple isochronous arcs connected to the ERLs, an interaction region design, a low energy ERL with a polarized electron source, and connecting beam lines.


* V. Litvinenko, proceedings from this conference.

 
MOPEA038 Gamma-Ray Source for Nuclear Resonance Fluorescence Based on Compton Storage Ring electron, laser, storage-ring, cavity 154
 
  • P. Gladkikh, E.V. Bulyak, V.A. Skomorokhov
    NSC/KIPT, Kharkov
  • T. Omori, J. Urakawa
    KEK, Ibaraki
 
 

Nuclear resonance fluorescence (NRF) is the one of the most promising methods of the nuclear waste management and of the modern technologies of the nonproliferation of nuclear weapons. There are a few proposals of the usage of NRF *,**. Yet linac and energy recovery linac are suggested as the electron source for the Compton scattering (CS) of the laser photons. The storage ring is capable to produce sufficiently higher beam intensity and is more effective since the electrons interact with the laser pulse many times. The storage ring with the electron energy from 240 to 530 MeV is proposed for the CS of 1.16 eV laser photons in the report. Maximal energy of the scattered gamma rays lies within range from 1 MeV to 5 MeV. It allows detecting of practically any isotope in analyzed objects. The specificity of the proposed storage ring is usage of the crab-crossing of the electron and laser beams. Due to crab-crossing we expect to obtain the gamma beam intensity approximately 5*1013 gammas/s for laser flash energy 5 mJ stored in the optical cavity. Both electron beam and gamma beam parameters are studied analytically and by simulation of the CS in the designed ring lattice.


* J. Pruet et al. Detecting clandestine material with nuclear resonance fluorescence. J. Appl. Phys., 99, 123102-1-11 (2006).
** R. Hajima et al. J. Nucl. Sci. Tech., vol. 45, pp. 441-451, 2008.

 
MOPEB001 Multi-function Corrector Magnet sextupole, quadrupole, power-supply, insertion 274
 
  • L.O. Dallin, D.G. Bilbrough
    CLS, Saskatoon, Saskatchewan
 
 

Storage rings require corrector magnets for a variety of tasks. Foremost are small dipole magnets for both horizontal and vertical correction. In light sources, for example, other corrector magnets are needed to compensate for the effect of changing insertion device operation points. These can include quadrupole, skew quadrupole, sextupole and skew sextupole corrections. As well octupole magnets may be desirable to improve dynamic aperture in small emittance lattices. One magnet can perform all these tasks. This is achieved by having separate windings with separate power supplies on an octopole yoke. The simultaneous excitation of any combination of modes can be achieved through superposition. Corrections are necessarily limited to avoid saturation effects that will degrade the superposition.

 
MOPEB014 Status of the PLS-II Magnet Design and Fabrication quadrupole, sextupole, dipole, electron 307
 
  • D.E. Kim, H.S. Han, Y.-G. Jung, K.R. Kim, H.-G. Lee, S.H. Nam, K.-H. Park, H.S. Suh
    PAL, Pohang, Kyungbuk
 
 

Pohang Light Source (PLS) is planning a major upgrade of the storage ring to meet the more demanding requirement from the synchrotron light users. The main features of the major upgrade are (1) increasing the electron beam energy from 2.5 GeV to 3.0 GeV for more higher energy X-ray photons, (2) decreasing the electron beam emittance from 1.89 nm to 5.8 nm to increase the photon brilliances, and (3) increasing the number of straight sections to install the insertion devices from 10 to 20 to meet the demand for insertion devices. in the upgraded PLS (PLS-II), there will be 24 combined function dipole magnets, 96 quadrupole magnets, and 144 sextupole magnets with some auxiliary magnets for electron beam injection. In this report, the physical design features, mechanical aspects of the magnet design are described.

 
MOPEC006 JMAD - Integration of MADX into the JAVA World optics, controls, quadrupole, status 465
 
  • K. Fuchsberger, V. Baggiolini, R. Gorbonosov, W. Herr, V. Kain, G.J. Müller, S. Redaelli, F. Schmidt, J. Wenninger
    CERN, Geneva
 
 

MADX (Methodical Accelerator Design) is the de-facto standard software for modeling accelerator lattices at CERN. This feature-rich software package is implemented and maintained in the programming languages C and FORTRAN. Nevertheless the controls environment of modern accelerators at CERN, e.g. of the LHC, is dominated by JAVA applications. A lot of these applications, for example for lattice measurement and fitting, require a close interaction with the numerical models, which are all defined by the use of the proprietary MADX scripting language. To close this gap an API to MADX for the JAVA programming language (JMAD) was developed. Already the current implementation provides access to a large subset of the MADX capabilities (e.g. twiss-calculations, matching or querying and setting arbitrary model parameters) without any necessity to define the models in yet another environment. This paper describes shortly the design of this project as well as the current status and some usage examples.

 
MOPEC024 RHIC BBLR Measurements in 2009 beam-losses, proton, emittance, interaction-region 510
 
  • R. Calaga, W. Fischer, G. Robert-Demolaize
    BNL, Upton, Long Island, New York
 
 

Long range beam-beam experiments were conducted during the Run 2009 in the yellow and the blue beams of the RHIC accelerator with DC wires. The effects of a long-range interaction with a DC wire on colliding and non-colliding bunches with the aid of orbits, tunes, and losses were studied. Results from distance and currents scans and an attempt to compensate a long-range interaction with a DC wire is presented.

 
MOPEC033 RHIC Performance as a 100 GeV Polarized Proton Collider in Run-9 luminosity, proton, polarization, emittance 531
 
  • C. Montag, L. Ahrens, M. Bai, J. Beebe-Wang, M. Blaskiewicz, J.M. Brennan, K.A. Brown, D. Bruno, R. Connolly, T. D'Ottavio, K.A. Drees, A.V. Fedotov, W. Fischer, G. Ganetis, C.J. Gardner, J.W. Glenn, H. Hahn, M. Harvey, T. Hayes, H. Huang, P.F. Ingrassia, J.P. Jamilkowski, A. Kayran, J. Kewisch, R.C. Lee, D.I. Lowenstein, A.U. Luccio, Y. Luo, W.W. MacKay, Y. Makdisi, N. Malitsky, G.J. Marr, A. Marusic, M.P. Menga, R.J. Michnoff, M.G. Minty, J. Morris, B. Oerter, F.C. Pilat, P.H. Pile, E. Pozdeyev, V. Ptitsyn, G. Robert-Demolaize, T. Roser, T. Russo, T. Satogata, V. Schoefer, C. Schultheiss, F. Severino, M. Sivertz, K. Smith, S. Tepikian, P. Thieberger, D. Trbojevic, N. Tsoupas, J.E. Tuozzolo, A. Zaltsman, A. Zelenski, K. Zeno, S.Y. Zhang
    BNL, Upton, Long Island, New York
 
 

During the second half of Run-9, the Relativistic Heavy Ion Collider (RHIC) provided polarized proton collisions at two interaction points with both longitudinal and vertical spin direction. Despite an increase in the peak luminosity by up to 40%, the average store luminosity did not increase compared to previous runs. We discuss the luminosity limitations and polarization performance during Run-9.

 
MOPEC034 Experience with Split Transition Lattices at RHIC acceleration, storage-ring, ion, optics 534
 
  • C. Montag, M. Blaskiewicz, J.M. Brennan, S. Tepikian
    BNL, Upton, Long Island, New York
 
 

During the acceleration process, heavy ion beams in RHIC cross the transition energy. When RHIC was colliding deuterons and gold ions during Run-8, lattices with different integer tunes were used for the two rings. This resulted in the two rings crossing transition at different times, which proved beneficial for the "Yellow" ring, the RF system of which is slaved to the "Blue" ring. For the symmetric gold-gold run in FY2010, lattices with different transition energies but equal tunes were implemented. We report the optics design concept as well as operational experience with this configuration.

 
MOPEC043 Error Study of a Novel Non-linear, Nonscaling FFAG dynamic-aperture, proton, resonance, acceleration 555
 
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • S.L. Sheehy
    JAI, Oxford
 
 

A novel nonlinear, nonscaling FFAG ring has been designed for proton and ion acceleration [1]. It can be used for proton and carbon therapy as well as a proton driver for various facilities such as a high intensity neutrino factory. The machine has novel features including variable energy extraction and a high repetition rate of about 1 kHz. Taking as an example the PAMELA proton ring, under study at the John Adams Institute in Oxford, we present results of an error study. A calculation of alignment tolerance is made, in which the effects of translational misalignments of the triplet magnets are included. The effect of misalignments on the dynamic aperture of the machine is investigated.


[1] S. L. Sheehy, K. J. Peach, H. Witte, D. J. Kelliher and S. Machida, Phys. Rev. ST Accel. Beams, 13 (2010) 040101

 
MOPEC044 A Fixed Field Alternating Gradient Accelerator With Long Straight Sections synchrotron, optics, focusing, dynamic-aperture 558
 
  • S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

The lattice of a Fixed Field Alternating Gradient (FFAG) accelerator normally has high symmetry. The whole ring consists of many identical cells which have a simple FODO, double or triplet focusing unit. There is, however, no real reason for an FFAG lattice to have high symmetry, except for a linear nonscaling design which relies on high symmetry to avoid betatron resonances. We propose an FFAG lattice design with a superperiod that makes it possible to have long straight sections for injection, extraction and rf cavities. We discuss how to introduce a superperiod structure. The impact on dynamic aperture, dispersion function, longitudinal dynamics as well as the advantage of having long straight sections will be presented.

 
MOPEC047 High Current Proton FFAG Accelerators space-charge, emittance, beam-losses, proton 564
 
  • R.J. Barlow, A.M. Toader, S.C. Tygier
    UMAN, Manchester
 
 

Accelerator Driven Subcritical Reactors require a high currents of energetic protons. We compute the limits imposed by space charge, and explore what can be achieved using various proposed FFAG lattices. Limitations due to beam losses and reliability are also discussed

 
MOPEC070 The Optimization of Beam Dynamics Design for CSNS/RCS dipole, collimation, injection, extraction 630
 
  • S. Wang, Q. Qin
    IHEP Beijing, Beijing
 
 

The accelerator of China Spallation Neutron Source (CSNS) consists of a low energy linac and a Rapid Cycling Synchrotron (RCS). The opimization of beam dynamics design for RCS and two beam transport line are introduced, and the details design and some simulation results are presented.

 
MOPEC081 The Concept Design of the CW Linac of the Project X cavity, linac, cryomodule, focusing 654
 
  • N. Solyak, E. Gianfelice-Wendt, I.G. Gonin, S. Kazakov, V.A. Lebedev, S. Nagaitsev, J.-F. Ostiguy, N. Perunov, G.V. Romanov, V.P. Yakovlev
    Fermilab, Batavia
 
 

The concept design of the 2.5 GeV superconducting CW linac of the Project X is discussed. The linac structure and break points for different cavity families are described. The results of the RF system optimization are presented as well as the lattice design and beam dynamics analysis.

 
MOPD010 Lattice of the NICA Collider Rings collider, optics, sextupole, proton 690
 
  • A.O. Sidorin, O.S. Kozlov, I.N. Meshkov, V.A. Mikhaylov, G.V. Trubnikov
    JINR, Dubna, Moscow Region
  • V.A. Lebedev, S. Nagaitsev
    Fermilab, Batavia
  • Y. Senichev
    FZJ, Jülich
 
 

Main element of the NICA facility is the collider equipped with stochastic and electron cooling systems to provide experiment with heavy ions like Au, Pb or U at energy from 1 to 4.5 GeV/u with average luminosity of the level of 1027 cm-2 s-1. The possible lattices providing the required parameters are discussed.

 
MOPD088 Resolution Studies of Inorganic Scintillation Screens for High Energy and High Brilliance Electron Beams electron, diagnostics, simulation, background 906
 
  • G. Kube, C. Behrens
    DESY, Hamburg
  • W. Lauth
    IKP, Mainz
 
 

Luminescent screens are widely used for particle beam diagnostics, especially in transverse profile measurements at hadron machines and low energy electron machines where the intensity of optical transition radiation (OTR) is rather low. The experience from modern linac based light sources showed that OTR diagnostics might fail even for high energetic electron beams because of coherence effects in the OTR emission process. An alternative way to overcome this limitation is to use luminescent screens, especially inorganic scintillators. However, there is only little information about scintillator properties for applications with high energetic electrons. Therefore a test experiment has been performed at the 855 MeV beam of the Mainz Microtron MAMI (University of Mainz, Germany) in order to study the spatial resolution. The results of this experiment will be presented and discussed in view of scintillator material properties and observation geometry.

 
MOPE062 Continuous Measurement and Control of Beta-Beating in the LHC pick-up, feedback, quadrupole, resonance 1119
 
  • R.J. Steinhagen, A. Boccardi, E. Calvo Giraldo, M. Gasior, J.L. Gonzalez, O.R. Jones
    CERN, Geneva
 
 

The beta function has a fundamental impact on the LHC performance and on the functioning of its machine protection and collimation systems. A new beta-beat diagnostic system, prototyped at the SPS, has been used to verify the time-dependent variations of the LHC lattice with unprecedented 1% beta-beta resolution and at a measurement bandwidth of about 1 Hz.

 
MOPE085 Rapid-cycling Synchrotron with Variable Momentum Compaction proton, dipole, collider, optics 1182
 
  • Y. Alexahin
    Fermilab, Batavia
  • D.J. Summers
    UMiss, University, Mississippi
 
 

There are conflicting requirements on the value of the momentum compaction factor during energy ramp in a synchrotron: at low energies it should be positive and sufficiently large to make the slippage factor small so that it is possible to work closer to the RF voltage crest and ensure sufficient RF bucket area, whereas at higher energies it should be small or negative to avoid transition crossing. In the present report we propose a lattice with variable momentum compaction factor and consider the possibility of using it in a high repetition rate proton driver for muon collider and neutrino factory.

 
TUPEA007 S-POD Experiments of Space-Charge-Dominated Beam Resonances resonance, plasma, ion, focusing 1339
 
  • H. Okamoto, K. Ito, H. Sugimoto
    HU/AdSM, Higashi-Hiroshima
  • H. Higaki
    Hiroshima University, Higashi-Hiroshima
  • S.M. Lund
    LLNL, Livermore, California
 
 

S-POD (Simulator for Particle Orbit Dynamics) is a tabletop, non-neutral plasma trap system developed at Hiroshima University for fundamental beam physics studies. The main components of S-POD include a compact radio-frequency quadrupole trap, various AC and DC power supplies, a vacuum system, a laser cooler, several diagnostics, and a comprehensive computer control system. A large number of ions, produced through the electron bombardment process, are captured and confined in the RFQ trap to emulate collective phenomena in space-charge-dominated beams traveling in periodic linear focusing lattices. This unique experiment is based on the isomorphism between a one-component plasma in the laboratory frame and a charged-particle beam in the center-of-mass frame. We here employ S-POD to explore the coherent betatron resonance instability which is an important issue in modern high-power accelerators. Ion loss behaviors and transverse plasma profiles are measured under various conditions to identify the parameter-dependence of resonance stopbands. Experimental observations are compared with PIC simulation results obtained with the WARP code.

 
TUPEA070 ECHARM - a Software for Calculation of Physical Quantities of Interest in Coherent Interaction of Relativistic Particles with Crystals plasma, scattering, simulation, FEL 1485
 
  • E. Bagli
    INFN-Ferrara, Ferrara
  • V. Guidi
    UNIFE, Ferrara
  • V.A. Maisheev
    IHEP Protvino, Protvino, Moscow Region
 
 

We present an analytical model to calculate the physical quantities of interest experienced by relativistic particles in their motion aligned with periodic complex atomic structures. Classical physics equations and the expansion of periodic functions as a Fourier series have been used for the calculation. This method allows calculating the contribution from all the planes and axes inside the crystal, in contrast to other simulation codes for which the motion is evaluated only on nearest neighbors atomic strings. Based on the calculation technique we have developed the "ECHARM" program, which allows calculating one- and two- dimensional averaged physical quantities of interest. The calculation holds for the main axes of any orthorhombic and tetragonal structures and for any orientation in the cubic structure. To underline the capability of the program, complex structures such as zeolites have been worked out. Based on the "ECHARM" code, simulation of the relativistic particle motion within complex structures has been developed. With this code it is possible to simulate the motion in bent crystal to study planar and axial channeling volume reflection.

 
TUPEB001 Lattice Design and Study Tools Regarding the Super-B Project simulation, radiation, photon, synchrotron 1512
 
  • F. Méot
    CEA, Gif-sur-Yvette
  • N. Monseu
    LPSC, Grenoble Cedex
 
 

Lattice design tools are being developed, and related beam and spin dynamics simulations are being performed, in the framework of the international collaboration regarding the super-B project. The present contribution reports on this work.

 
TUPEB004 Super-B Lattice Studies emittance, injection, dipole, sextupole 1521
 
  • Y. Nosochkov, W. Wittmer
    SLAC, Menlo Park, California
  • M.E. Biagini, P. Raimondi
    INFN/LNF, Frascati (Roma)
  • P.A. Piminov, S.V. Sinyatkin
    BINP SB RAS, Novosibirsk
 
 

The Super-B asymmetric e+e- collider is designed for 1036 cm-2sec-1 luminosity and beam energies of 6.7 and 4.18 GeV for e+ and e-, respectively. The machine will have the High and Low Energy Rings (HER and LER), and one Interaction Point (IP) with 60 mrad crossing angle. The INFN-LNF at Frascati is one of the proposed sites, and a lattice for short 1.3 km rings fitting to this site has been designed. The two rings are radially separated by 2 m except near the IP and in the dogleg on the opposite side of the rings. The injection sections and RF cavities are included. The lattice is optimized for a low emittance required for the desired high luminosity. Final Focus chromaticity correction is optimized for large transverse and energy acceptance. The "crab waist" sextupoles are included for suppression of betatron resonances induced at the IP collisions with large Piwinski angle. The LER spin rotator sections provide longitudinal polarization for the electron beam at IP. The lattice is flexible for tuning the design parameters and compatible with reusing the PEP-II magnets, RF cavities and other components. Design criteria and details on the lattice implementation are presented.

 
TUPEB021 Conceptual Design of the Muon Collider Ring Lattice sextupole, collider, dynamic-aperture, beam-beam-effects 1563
 
  • Y. Alexahin, E. Gianfelice-Wendt, A.V. Netepenko
    Fermilab, Batavia
 
 

Muon collider is a promising candidate for the next energy frontier machine. However, in order to obtain peak luminosity in the 1035/cm2/s range the collider lattice design must satisfy a number of stringent requirements, such as low beta at IP (beta*<1 cm), large momentum acceptance and dynamic aperture and small value of the momentum compaction factor. Here we present a particular solution for the interaction region optics whose distinctive feature is a three-sextupole local chromatic correction scheme. Together with a new flexible momentum compaction arc cell design this scheme allows to satisfy all the above-mentioned requirements and is relatively insensitive to the beam-beam effect.

 
TUPEB045 Correction of the Chromaticity up to Second Order for MEIC sextupole, collider, quadrupole, electron 1629
 
  • H. K. Sayed
    CASA, newport news
  • S.A. Bogacz, Y. Roblin
    JLAB, Newport News, Virginia
 
 

The proposed electron collider lattice exhibits low β- functions at the Interaction Point (IP) (βx∗100mm − βy∗ 20 mm) and rather large equilibrium momentum spread of the collider ring (δp/p = 0.00158). Both features make the chromatic corrections of paramount importance. Here the chromatic effects of the final focus quadruples are cor- rected both locally and globally. Local correction features symmetric sextupole families around the IP, the betatron phase advances from the IP to the sextupoles are chosen to eliminate the second order chromatic aberration. Global interleaved families of sextupoles are placed in the figure-8 arc sections, and non-interleaved families at straight sec- tion making use of the freely propagated dispersion wave from the arcs. This strategy minimizes the required sex- tupole strength and eventually leads to larger dynamic aper- ture of the collider. The resulting spherical aberrations induced by the sextupoles are mitigated by design; the straight and arc sections optics features an inverse identity transformation between sextupoles in each pair.

 
TUPEB075 Preliminary results of the crystal collimation test in UA9 collimation, radiation, beam-losses, simulation 1695
 
  • D. Mirarchi, G. Cavoto
    INFN-Roma, Roma
  • R. Losito, W. Scandale
    CERN, Geneva
  • A.M. Taratin
    JINR, Dubna, Moscow Region
 
 

We present a detailed analysis of the beam loss data collected at the SPS during the 2009 machine developments devoted to test crystal collimation. Scintillator counters and Gas electron multiplier detectors were installed in special points to detect the effect of inelastic interaction of protons with the crystals in various orientation with respect to the beam. Clear correlations of the counting rates with the crystal positions and orientation were detected during the data-taking and were crucial to put the crystal in optimal channeling position. For one of the crystal the pattern of losses showed evidence of several planar and axial channeling conditions.

 
TUPEC040 Optimal Twiss Parameters for Top Off Injection in a Synchrotron Light Source injection, storage-ring, multipole, emittance 1814
 
  • R.P. Fliller
    BNL, Upton, Long Island, New York
 
 

Injection into a ring requires that the injected beam be optimally matched to the storage ring lattice. For on axis injection this requires that the twiss functions of the transfer line match the twiss functions of the lattice. When injection off axis, as is done in light sources for top off injection, the goal is to use the minimum phase space area in the storage ring. A. Streun* has given an analytical method to compute the twiss functions for top off injection into the SLS where injection occurs at a beam waist. We have extended his theory to include cases where there is no beam waist. A simple analytical formula is not possible in this case, however we give an algorithm to compute the twiss parameters of the injected beam given the storage ring lattice. We also compute the twiss functions for a variety of cases for the NSLS-II storage ring.


* A. Streun. "SLS booster-to-ring transfer line optics for optimum injection effciency". Technical Note SLS-TME-TA-2002-0193. May 27, 2005.

 
TUPEC058 Beam Dynamics in NS-FFAG EMMA with Dynamical Maps closed-orbit, betatron, acceleration, transverse-dynamics 1856
 
  • Y. Giboudot, R. Nilavalan
    Brunel University, Middlesex
  • T.R. Edgecock
    STFC/RAL, Chilton, Didcot, Oxon
  • A. Wolski
    The University of Liverpool, Liverpool
 
 

The Non Scaling Fixed Field Alternating Gradient EMMA has a compact linear lattice. Effect of Fringe Field on the beam has to be studied carefully. A numerical magnetic field map is generated by magnet measurements or magnet design softwares. We developed a technique that produces from the numerical field map, a dynamical map for a particle travelling in the entire EMMA cell for a reference energy without acceleration. Since the beam dynamics change with energy, a set of maps have been produce with different reference energies between 10 and 20MeV. For each reference energy, simulated tune and time of flight (TOF) have been compared with results in Zgoubi - tracking directly through numerical field map. The range of validity of a single map has been investigated by tracking particle with large energy deviation. From that, a sensible acceleration scheme has been implemented.


yoel.giboudot@stfc.ac.uk

 
TUPEC060 Serpentine: A New Code for Particle Tracking quadrupole, simulation, sextupole, alignment 1862
 
  • S. Molloy, S.T. Boogert
    Royal Holloway, University of London, Surrey
 
 

Serpentine is a Python library, written for the purpose of simulating charged particle accelerators. It has been written to allow for the simulation of both rings and single-shot machines in a light-weight way (i.e. without requiring significant computational resources for typical calculations, such as the determination of transfer matrices, or matching of Twiss parameters), and has been structured to be highly modular (i.e. allowing extension of the simulations to include effects not already included in the base installation). Through the use of the Universal Accelerator Parser (UAP), Serpentine has no need for a new lattice representation, and allows access to any lattice format understood by UAP. The operation of this code on several complex accelerator designs is demonstrated.

 
TUPEC062 Advanced Multi-program GUI for Accelerator Modeling simulation, quadrupole, collider, linear-collider 1868
 
  • T.J. Roberts
    Muons, Inc, Batavia
  • D.M. Kaplan
    Illinois Institute of Technology, Chicago, Illinois
 
 

There are dozens of programs for designing and modeling accelerator systems, most of which have their own language for describing the system. This means a designer must spend considerable time learning the languages of different programs and converting system descriptions among them. This paper describes a project to develop a new language for accelerator modeling, together with a portable suite of programs to implement it. These programs will assist the user while editing, visualizing, developing, simulating, and sharing models of accelerator components and systems. This suite is based on a Graphical User Interface (GUI) that will permit users to assemble their system graphically and then display it and check its sanity visually, even while using modeling programs that have no graphical or visualization capabilities. Incorporating the concept of libraries as a primary component of the language will encourage collaboration among geographically diverse teams. The requirements for developing this language and its tools will be based on generality, flexibility, extensibility, portability, usability, and sharability.

 
TUPEC080 Recent Enhancements to the ORBIT Code focusing, multipole, simulation, emittance 1901
 
  • J.A. Holmes
    ORNL, Oak Ridge, Tennessee
 
 

At an age of twelve years, the collective beam dynamics particle tracking code, ORBIT, is considered mature. Even so, we continue to enhance ORBIT's capabilities. Two such enhancements are reported here. The first enhancement allows for the use of time dependent waveforms for the strengths of all magnetic elements, a capability that previously was limited to kickers and to RF cavities. This capability should prove very useful for applications to synchrotrons, in which tunes are often manipulated during acceleration. The second enhancement provides an internal calculation of the lattice functions. Previously, these had to be read from an external file, but given the capability of dynamically programming the lattice magnet strengths, it is extremely useful to be able to calculate the lattice functions on demand. Examples illustrating these new ORBIT capabilities will be presented.

 
TUPEC084 New Particle-in-cell Code for Numerical Simulation of Coherent Synchrotron Radiation simulation, electron, synchrotron, synchrotron-radiation 1913
 
  • B. Terzić
    CASA, newport news
  • R. Li
    JLAB, Newport News, Virginia
 
 

We present early stage of a new code for self-consistent, 2D simulations of beam dynamics affected by CSR. The code is of the particle-in-cell variety: the beam bunch is sampled by macroparticles, which are deposited on the grid; the corresponding forces on the grid are then computed using retarded potentials according to causality, and interpolated so as to advance the particles in time. The retarded potentials are evaluated by integrating over the 2D path history of the bunch, with the charge and current density at the retarded time obtained from interpolation of the particle distributions recorded at discrete timesteps. The code is benchmarked against analytical results obtained for a rigid-line bunch. We also outline the features and applications which are currently being developed.

 
TUPD011 Intrabeam Scattering at Low Temperature Range scattering, ion, plasma, simulation 1943
 
  • P.-CH. Yu, J. Wei
    TUB, Beijing
  • Z.Q. He
    Tsinghua University, Beijing
  • H. Okamoto
    HU/AdSM, Higashi-Hiroshima
  • A. Sessler
    LBNL, Berkeley, California
  • Y. Yuri
    JAEA/TARRI, Gunma-ken
 
 

During the beam crystallization process, the main heating source is Intra-beam scattering (IBS), in which the Coulomb collisions among particles lead to a growth in the 6D phase space volume of the beam. The results of molecular dynamics (MD) simulation have shown an increase of heating rate as the temperature is increased from absolute zero, but then a peak in the heating rate, and subsequent decrease with ever increasing temperature*. This phenomenon has been carefully studied by Y. Yuri, H. Okamoto, and H. Sugimoto**. On the other hand, in the traditional IBS theory valid at high temperatures, heating rate is monotonically increasing as the temperature becomes lower***. In this paper we attempt to understand the "matching" at low temperatures between the MD results and traditional IBS theory, by including many body effects in the traditional IBS theory. In particular the Debye shielding is included. We shall present how the traditional theory is modified by shielding, and show how this effect improves the "matching" with the results from MD.


* J. Wei, H. Okamoto, and A. Sessler, Phys. Rev. Lett. 80, 2606
** Y.Yuri, H. Okamoto, and H. Sugimoto, J. Phys. Soc. Jpn. 78, 124501
***A. Piwinski, Lect. Notes Phys. 296, 297 (1988)

 
TUPD020 Studies of Space Charge Effects in the Proposed CERN PS2 emittance, space-charge, synchrotron, simulation 1964
 
  • J. Qiang, R.D. Ryne
    LBNL, Berkeley, California
  • R. De Maria
    BNL, Upton, Long Island, New York
  • A. Macridin, P. Spentzouris
    Fermilab, Batavia
  • Y. Papaphilippou
    CERN, Geneva
  • U. Wienands
    SLAC, Menlo Park, California
 
 

A new proton synchrotron, the PS2, is under design study to replace the the current proton synchrotron at CERN for the LHC upgrade. Nonlinear space charge effects could cause significant beam emittance growth and particle losses and limit the performance of the PS2. In this paper, we report on studies of the potential space-charge effects at the PS2 using three-dimensional self-consistent macroparticle tracking codes, IMPACT, MaryLie/IMPACT, and Synergia. We will present initial benchmark results among these codes. Effects of space-charge on the emittance growth, especially due to synchrotron coupling, and the aperture sizes will also be discussed.

 
TUPD021 Method to Extract Transfer Maps in the Presence of Space Charge in Charged Particle Beams space-charge, resonance, electron, multipole 1967
 
  • E.W. Nissen, B. Erdelyi
    Northern Illinois University, DeKalb, Illinois
  • S.L. Manikonda
    ANL, Argonne
 
 

This research involves a method for combining the intricate diagnostic tools for calculating quantities of interest such as tunes, dispersion and resonances from the single particle map of the system, with an accurate approximation of space charge effects on the beam. The space charge calculation involves a novel method of potential integration which allows for rapid Taylor expansion around singularities. This will allow for an accurate computation of space charge induced tune shifts and resonances, as well as allowing for experimental setups to discriminate between space charge caused issues, and lattice caused issues. The code used was COSY Infinity 9.0 which uses Differential Algebras to determine numerical derivatives to arbitrary order, and Normal Form methods to extract information from the map. The effects of space charge are added to the map using Strang splitting. External confounding factors such as the earths magnetic field are also addressed.

 
TUPD029 Coherent Instability Thresholds and Dynamic Aperture with Octupoles and Nonlinear Space-Charge in the SIS100 Synchrotron octupole, space-charge, simulation, impedance 1988
 
  • V. Kornilov, O. Boine-Frankenheim
    GSI, Darmstadt
  • V.V. Kapin
    ITEP, Moscow
 
 

Octupole magnets can be used as a passive cure against transverse collective instabilities. The octupole field creates a betatron frequency spread due to amplitude-dependent tune shift and thus enhances Landau damping. The drawback is the reduction of the dynamic aperture (DA). Ultimately, a balance between collective damping and DA must be found. Here we analyse the transverse coherent instability thresholds in SIS100 with octupoles and nonlinear space-charge taken into account. As the major impedance sources at low frequencies, the resistive wall and the kickers are considered. A coasting beam is assumed, which results in a conservative stability estimation. On the other hand, we simulate the DA of the SIS100 lattice using the MADX code, with systematic multipole errors, random multipole errors, and closed-orbit errors taken into account.

 
TUPD102 Magnet Optics and Beam Dynamics of BERLinPro linac, optics, multipole, cavity 2135
 
  • M. Abo-Bakr, B.C. Kuske, A.N. Matveenko
    Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, Elektronen-Speicherring BESSY II, Berlin
 
 

The Helmholtz Zentrum Berlin (HZB) is proposing to build an Energy Recovery Linac Prototype, called BERLinPro, at its site in Berlin Adlershof. A gun test stand for a superconducting RF gun is already under construction at HoBiCaT. In this paper we concentrate on the recirculator part of the ERL and discuss the ERL requirements to the magnet optics. The current design of the magnet lattice will be described and main parameters and simulation results introduced. Since BERLinPro aims to demonstrate high current operation at short pulses according optics aspects will be also discussed. The focus here will be on longitudinal phase space manipulations and lattice layout options, suppressing the BBU instability and increasing its threshold currents.

 
TUPE098 Cornell Energy Recovery Linac Lattice and Layout undulator, simulation, linac, optics 2356
 
  • C.E. Mayes, G.H. Hoffstaetter
    CLASSE, Ithaca, New York
 
 

The current status of the lattice and layout for the proposed Cornell Energy Recovery Linac lightsource is presented. This design is centered about a new hard X-ray user facility to be located on Cornell's campus, and is adapted to the local topography in order to incorporate the existing CESR tunnel and Wilson Laboratory. Nonlinear charged-particle optics for this new machine have been designed and analyzed. The lattice is populated with various components for the appropriate accelerator physics requirements for orbit, bunch length, and emittance growth control, including a vacuum system compatible with rest-gas-scattering limits, a collimation system for halo from effects like Touschek scattering, and correction coils and BPMs for sub-micron beam stabilization. We also show calculations for an additional bunch compression mode, which compresses 19~pC bunches at a 1.3~GHz repetition rate to 25~fs.

 
WEOBRA01 Benchmarking of the NTRM Method on Octupolar Nonlinear Components at the CERN-SPS Synchrotron octupole, resonance, sextupole, simulation 2435
 
  • G. Franchetti, A.S. Parfenova
    GSI, Darmstadt
  • R. Tomás, G. Vanbavinckhove
    CERN, Geneva
 
 

The measurement of synchrotron nonlinear components is an essential step for devising an effective compensation scheme for improving machine performances. A validation test of a recently proposed method called nonlinear tune response matrix (NTRM) for measuring circular accelerator nonlinear components is undergoing in a CERN-GSI joint effort. The test consists in the attempt of reconstructing few controlled octupolar components in the SPS synchrotron. In this proceeding we report on the SPS benchmarking experiment and discuss the performances the NTRM method applied to this measurements.

 

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WEPEA006 SIRIUS (Br): A New Brazilian Synchrotron Light Source dipole, emittance, synchrotron, dynamic-aperture 2481
 
  • L. Liu, X.R. Resende, A.R.D. Rodrigues
    LNLS, Campinas
 
 

We report on the status of SIRIUS (BR), the new 3 GeV synchrotron light source currently being designed at the Brazilian Synchrotron Light Laboratory (LNLS) in Campinas, Brazil. The new light source will consist of a low emittance storage ring based on the use of permanent magnet technology for the dipoles. An innovative approach is adopted to enhance the performance of the storage ring dipoles by combining low field (0.5 T) magnets for the main beam deflection and a short slice of high field magnet. This short slice will create a high bending field (2.0 T) only over a short longitudinal extent, generating high critical photon energy with modest energy loss from the complete dipole. There are several attractive features in this proposal, including necessity for lower RF power, less heating of the vacuum chambers and possibility to reduce the beam emittance by placing the longitudinal field gradient at a favorable place.

 
WEPEA011 Double Low Beta Straight Section for Dual Canted Undulators at SOLEIL quadrupole, resonance, optics, sextupole 2496
 
  • A. Loulergue, C. Benabderrahmane, F. Bouvet, P. Brunelle, M.-E. Couprie, J.-C. Denard, J.-M. Filhol, C. Herbeaux, P. Lebasque, V. Leroux, A. Lestrade, O. Marcouillé, J.L. Marlats, F. Marteau, T. Moreno, A. Nadji, L.S. Nadolski, F. Polack, A. Somogyi, M.-A. Tordeux
    SOLEIL, Gif-sur-Yvette
 
 

SOLEIL is the French 2.75 GeV high brilliance third generation synchrotron light source delivering photons to 20 beamlines with a current of 400 mA in multibunch or hybrid modes, and 60 mA in 8 bunch mode. There are already 17 insertion devices installed and 9 others are planned in the next 2 coming years. Among them, two canted in vacuum insertion devices are planned, for the Nanoscopium and Tomography beamlines, and will be accommodated in a 12 m long straight section, with a 6.5 mrad separation angle. These ~150 m long beamlines will exploit the high brilliance and coherence characteristics of the X-ray (5-20 keV) beam both for diffraction limited focusing and for contrast formation. To provide low vertical beta functions at each undulator, an extra triplet of quadrupoles was added in the middle of the section. We present here the lattice implementation footprint, the different working point under investigations as well as the first results of the measurements on the machine performances.

 
WEPEA014 Optics calibration at the MLS and at BESSY II optics, synchrotron, quadrupole, radiation 2505
 
  • P.O. Schmid, P. Kuske
    Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, Berlin
  • D.B. Engel, J. Feikes, R. Müller, G. Wüstefeld
    Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, Elektronen-Speicherring BESSY II, Berlin
 
 

In this paper we present the results of our studies employing LOCO and MML for optics calibration at the MLS and at the BESSY II storage rings. Both the standard user modes and dedicated low alpha modes were analysed.

 
WEPEA023 Proposal for a 3rd Generation National Iranian Synchrotron Light Source synchrotron, booster, emittance, storage-ring 2532
 
  • J. Rahighi
    IPM, Tehran
 
 

An overview of the 3 GeV Synchrotron radiation source, which is under design in Iran will be presented with emphasis on site location studies, user demands and general parameters of the machine. The background to the proposed facility and different aspects of the machine design also is reported. Operating this third generation light source with 3 GeV storage ring and beam currents of up to 400mA, will result in a source of very intense light over a broad range of photon energies from the IR to hard X-rays to a community that is expected to exceed 500 users a few years after the start of operation in 2015 .

 
WEPEA032 Design Study of a very Low-emittance Storage Ring for the Future Upgrade Plan of SPring-8 emittance, sextupole, storage-ring, dynamic-aperture 2555
 
  • K. Soutome, H. Ohkuma, J. Schimizu, Y. Shimosaki, M. Takao
    JASRI/SPring-8, Hyogo-ken
 
 

The SPring-8 storage ring has been operated for more than ten years and provided brilliant hard X-ray radiation to users. In recent years there are some discussions on upgrade plans of existing synchrotron radiation facilities and proposals of new facilities. In these the target brilliance of photons is set to be comparable or even higher, in some energy range, than that of the present value of SPring-8. At SPring-8 a design study of a new storage ring is now in progress for the future upgrade plan. The lattice structure will be changed from the present double-bend type to the multi-bend one, keeping the source position of all insertion devices unchanged. The emittance will be lowered from the present value of 3.4nmrad at 8GeV to 0.4nmrad at 6GeV (or 0.8nmrad at 8GeV) in the case of triple-bend lattice and 0.2nmrad at 6GeV (or 0.3nmrad at 8GeV) in the case of quadruple-bend lattice. We will report the present state of our preliminary work on lattice design. Nonlinear resonance correction to enlarge the dynamic aperture for on- and off-momentum electrons will also be discussed.

 
WEPEA041 Emittance Growth Estimation due to Intrabeam Scattering in Hefei Advanced Light Source(HALS) Storage Ring emittance, wiggler, damping, scattering 2582
 
  • W. Fan, G. Feng, D.H. He, W. Li, L. Wang, S.C. Zhang
    USTC/NSRL, Hefei, Anhui
 
 

Hefei Advanced Light Source(HALS) will be a high brightness light source with about 0.2nmrad emittance at 1.5GeV and about 400m circumference. To enhance brilliance, very low beam emittance is required. High brightness demand and relative low energy will make emittance a critical issue in ring design. Intra-beam scattering(IBS) is usually thought a fundamental limitation to achieve low emittance. Here we preliminarily estimate the emittance growth due to IBS for the temporary lattice design of HALS based on Piwinski and Bjorken-Mtingwa theories, and discuss the effect of implementation of damping wiggler and harmonic cavity to lower the emittance.

 
WEPEA042 Lattice Design and Beam Lifetime Study for HLS St01orage Ring Upgrade Project radiation, synchrotron, emittance, storage-ring 2585
 
  • G. Feng, W. Fan, W.W. Gao, W. Li, L. Wang, H. Xu, S.C. Zhang
    USTC/NSRL, Hefei, Anhui
 
 

HLS (Hefei Light Source) is a dedicated synchrotron radiation research facility, whose emittance is relatively large. In order to improve performance of the machine, especially getting higher brilliance synchrotron radiation and increasing the number of straight sections for insertion devices, an upgrade project is on going. A new low emittance lattice, which keeps the circumference of the ring no changing, has been studied and presented in this paper. For the upgrade project, a new ring will be installed on current ground settlement of HLS and all of the magnets will be reconstructed. After optimization, two operation modes have been chosen for different users. Nonlinear dynamics shows that dynamic aperture for on-momentum and off-momentum particle is large enough. Beam lifetime has also been studied. Calculation results proves that expected beam lifetime about 8.5 hours can be obtained with a fourth harmonic cavity operation.

 
WEPEA043 The Upgrade Project of Hefei Light Source (HLS) emittance, injection, storage-ring, brilliance 2588
 
  • L. Wang, W. Fan, G. Feng, W.W. Gao, W. Li, H. Xu, S.C. Zhang
    USTC/NSRL, Hefei, Anhui
 
 

The Hefei Light Source is composed of an 800 MeV storage ring, a 200 MeV electron linac and transfer line, which was designed and constructed twenty years ago. Several factors limit the performance of HLS, for example, less number of insertion devices and large beam emittance. To meet the requirements of synchrotron radiation users, an upgrade project of HLS will be carried out in the next two years. Several sub-systems will be renewed, such as magnet system, power supply, beam diagnostics, vacuum system, etc. The upgrade scheme is described in this paper, including magnet lattice design, nonlinear performance, collective effects,beam injection, orbit detection and correction, injector, etc.

 
WEPEA048 A Design Approach of the Beam Optics in the Complex Storage Ring optics, storage-ring, emittance, quadrupole 2597
 
  • S.Q. Tian, H.H. Li, X.Y. Sun, M.Z. Zhang, W.Z. Zhang
    SINAP, Shanghai
 
 

Beam optics design is a crucial issue in modern synchrotron radiation facility. A design approach of the beam optics is presented here. It provides much convenience for effectively exploring achievable linear optics and globally investigating flexibility of a complex lattice with super-periodicity. Low-ε optics and low-αC optics are emphasized, and the SSRF storage ring is taken as a test lattice.

 
WEPEA056 Beam Optics Measurements During the Commissioning of the ALBA Booster booster, injection, quadrupole, closed-orbit 2612
 
  • G. Benedetti, D. Einfeld, Z. Martí, M. Muñoz
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The commissioning of the booster for the synchrotron light source ALBA should take place in the period December 2009-January 2010. In this paper, the beam dynamics aspects of the commissioning are described, including the studies performed, the main problems find during the commissioning and a comparison of the measured beam parameters to the design one. A description of the software tools used and developed for the task is included.

 
WEPEA058 Status of the MAX IV Storage Rings storage-ring, sextupole, injection, linac 2618
 
  • S.C. Leemann, J. Ahlback, Å. Andersson, M. Eriksson, M.A.G. Johansson, L.-J. Lindgren, M. Sjöström, E.J. Wallén
    MAX-lab, Lund
 
 

In 2009 the MAX IV facility was granted funding by Swedish authorities. Construction of the facility will begin this summer and user operation is expected by 2015. MAX IV will consist of a 3.4 GeV linac as a driver for a short-pulse radiation facility (with planned upgrade to a seeded/cascaded FEL) as well as an injector for two storage rings at different energies serving user communities in separate spectral ranges. Thanks to a novel compact multibend-achromat design, the 3 GeV ring will deliver a 500 mA electron beam with a horizontal emittance below 0.3 nm rad to x-ray insertion devices located in 19 dispersion-free 5 m straight sections. When the 3 GeV ring goes into operation in 2015 it is expected to become the highest electron-brightness storage ring light source worldwide. The 1.5 GeV ring will serve as a replacement for both present-day MAX II and MAX III storage rings. Its below 6 nm rad horizontal emittance electron beam will be delivered to infrared and UV insertion devices in twelve 3.5 m straight sections. We report on design progress for the two new storage rings of the MAX IV facility.

 
WEPEA059 Energy Acceptance and Touschek Lifetime Calculations for the TPS Storage Ring coupling, emittance, optics, multipole 2621
 
  • H.-J. Tsai, H.-P. Chang, M.-S. Chiu, P.J. Chou, C.-C. Kuo, W.T. Liu, G.-H. Luo, F.H. Tseng, C.H. Yang
    NSRRC, Hsinchu
 
 

Touschek scattering is an important beam lifetime limiting effect for the TPS storage ring due to several challenges such as low emittance, small physical aperture and large second-order momentum compaction factor (nonlinear longitudinal motion). The Touschek relevant energy acceptance is determined by these challenges, therefore a reliable estimate of the Touschek lifetime is essential. We obtained Touschek induced betatron oscillation amplitudes in three sections (LS, SS and ARC) and RF bucket acceptance analytically and with simulations. In this paper, we present the energy acceptance and Touschek lifetime calculations for the TPS storage ring in the cases for different chromaticity settings, ID chamber limitations, magnet multipole field errors and optics correction effects.

 
WEPEA060 An Update of the Lattice Design of the TAC Proposed Synchrotron Radiation and Insertion Devices storage-ring, radiation, undulator, insertion 2624
 
  • K. Zengin, A.K. Çiftçi, R. Çiftçi
    Ankara University, Faculty of Sciences, Tandogan/Ankara
 
 

The Turkish Accelerator Center (TAC) is a project for accelerator based fundamental and applied researches supported by Turkish State Planning Organization (TSPO). The proposed synchrotron radiation facility of TAC was consisted of 3.56 GeV positron ring for a third generation light source. In the first study, it was shown that the insertion devices with the proposed parameter sets produce maximal spectral brightness to cover 10 eV - 100 keV photon energy range. Now, in this study it is considered that the electron beam energy will be increased to 4.5 GeV, in order to obtain more brightness light and wide energy spectrum range, also the beam emittance reduced to 1 nm.rad.

 
WEPEA068 Pulsed Multipole Injection for the ALS Upgrade injection, kicker, multipole, sextupole 2642
 
  • D. Robin, G.C. Pappas, C. Sun
    LBNL, Berkeley, California
  • Z.K. Fisher
    MIT, Cambridge, Massachusetts
 
 

We have developed computer models for a pulsed-multipole magnet injection scheme for the Advanced Light Source (ALS) at Lawrence Berkeley National Lab. The multipole kicker injection scheme is further shown to be com- patible with the ALS in combination with a magnet lattice that has a low beta-function in the injection straight. Since traditional injection schemes are not compatible with such optimized low beta lattices, implementing the new injection scheme opens up several new possibilities. For instance, the adoption of a low beta lattice can greatly increase brightness due to the better matching of photon and electron beam emittances. This document explains the principles of the injection and the simulations we performed to show that the concept is sound.

 
WEPEA070 Status of the Low Emittance Upgrade of the Advanced Light Source emittance, brightness, sextupole, insertion 2645
 
  • C. Steier, B.J. Bailey, A. Biocca, A. Madur, H. Nishimura, G.J. Portmann, S. Prestemon, D. Robin, S.L. Rossi, F. Sannibale, T. Scarvie, D. Schlueter, W. Wan, L. Yang
    LBNL, Berkeley, California
 
 

The Advanced Light Source is one of the earliest 3rd generation light sources. With an active upgrade program it has remained competitive over the years. The latest in a series of upgrades is a lattice upgrade project that was started in 2009. When it will be completed, the ALS will operate with a horizontal emittance of 2.2 nm and an effective emittance of 2.6 nm. Combined with the high current of 500 mA and the small vertical emittance the ALS already operates at this upgrade will keep it competitive for years to come. The presentation will present the status of the upgrade, including beam dynamics studies and lattice optimizations as well as the magnet design and status.

 
WEPEA072 An Extension of Cornell's Energy Recovery Linac for Compressed High-charge Bunches linac, emittance, dipole, sextupole 2651
 
  • F.A. Laham
    Cornell University, Ithaca, New York
  • G.H. Hoffstaetter, C.E. Mayes, J.R. Thompson
    CLASSE, Ithaca, New York
 
 

The proposed Cornell Energy Recovery Linac (ERL) is designed for bunches of 77pC and 100mA whose energy is recovered. However, the ERL linac can also be used for larger bunch charges of reduced average current whose energy does not have to be recovered. The proposed Cornell ERL lightsource currently uses a split linac arrangement connected by a turnaround arc. In order to avoid the detrimental effects of Coherent Synchrotron Radiation (CSR) in this arc, a high charge (1nC) bunch must remain relatively long (2ps), and be compressed at high energy (5GeV). An appropriate bunch compressor must take second order effects into account, which adds complications for the large energy spread associated with compression to 100fs or less. We have therefore designed a very simple four dipole bunch compressor at high energy, which uses second order time of flight terms in the turnaround arc rather than in the bunch compressor itself. This design is tested using particle tracking simulations incorporating CSR, as well as magnetic field errors and misalignments.

 
WEPEA073 Lattice Development for PEP-X High Brightness Light Source injection, sextupole, emittance, dynamic-aperture 2654
 
  • Y. Nosochkov, Y. Cai, M.-H. Wang
    SLAC, Menlo Park, California
 
 

Design of PEP-X high brightness light source machine is under development at SLAC. The PEP-X is a proposed replacement of the PEP-II in the existing 2.2 km tunnel. Two of the PEP-X six arcs contain DBA type lattice providing 30 dispersion free straights suitable for 3.5 m long undulators. The lattice contains TME cells in the other four arcs and a 90 m wiggler in a long straight section yielding an ultra low horizontal emittance of ~0.1 nm-rad at 4.5 GeV for a high brightness. The recent lattice modifications further increase the predicted brightness and improve beam dynamic properties. The standard DBA cells are modified into supercells for providing low beta undulator straights. The DBA and TME lattice parameters are better optimized. Harmonic sextupoles are added into the DBA arcs to minimize the sextupole driven resonance effects and amplitude dependent tune shift. Finally, the injection scheme is changed from vertical to horizontal plane in order to avoid large vertical amplitudes of injected beam within small vertical aperture of undulators.

 
WEPEA074 A Baseline Design for PEP-X: an Ultra-low Emittance Storage Ring emittance, brightness, scattering, undulator 2657
 
  • Y. Cai, K.L.F. Bane, K.J. Bertsche, A. Chao, R.O. Hettel, X. Huang, Z. Huang, C.-K. Ng, Y. Nosochkov, A. Novokhatski, T. Rabedeau, J.A. Safranek, G.V. Stupakov, L. Wang, M.-H. Wang, L. Xiao
    SLAC, Menlo Park, California
 
 

Over the past year, we have worked out a baseline design for PEP-X, as an ultra-low emittance storage ring that could reside in the existing 2.2-km PEP-II tunnel. The design features a hybrid lattice with double bend achromat cells in two arcs and theoretical minimum emittance cells in the remaining four arcs. Damping wigglers reduce the horizontal emittance to 86 pm-rad at zero current for a 4.5 GeV electron beam. At a design current of 1.5 A, the horizontal emittance increases, due to intra-beam scattering, to 164 pm-rad when the vertical emittance is maintained at a diffraction limited 8 pm-rad. The baseline design will produce photon beams achieving a brightness of 1022 (ph/s/mm2/mrad2/0.1% BW) at 10 keV in a 3.5-m conventional planar undulator. Our study shows that an optimized lattice has adequate dynamic aperture, while accommodating a conventional off-axis injection system. In this paper, we will present the study of the lattice properties, nonlinear dynamics, intra-beam scattering and Touschek lifetime, and collective instabilities. Finally, we discuss the possibility of partial lasing at soft X-ray wavelengths using a long undulator in a straight section.

 
WEPEA076 NSLS-II Lattice Optimization with Non-zero Chromaticity resonance, sextupole, damping, quadrupole 2663
 
  • W. Guo, S. Krinsky, L. Yang
    BNL, Upton, Long Island, New York
 
 

Chromaticity is usually set to non-zero value at the third generation light sources to cure the intensity induced instabilities. It is effective in suppressing the beam centroid oscillation; however, it is repeatedly reported that the beam lifetime decreases significantly when chromaticity goes up. This is probably due to the crossing of resonance lines by the enlarged tune footprint. In this paper we optimize the NSLS-II lattice at different positive chromaticity settings. The tune footprint is adjusted to fit in the stable region divided by the strong resonance lines. Tracking results show that we can maintain a lifetime similar to that of the zero-chromaticity lattice solutions.

 
WEPEA077 Physics Considerations and Specifications for the NSLS-II Magnets multipole, quadrupole, sextupole, dynamic-aperture 2666
 
  • W. Guo, S.L. Kramer, S. Krinsky, B. Nash, J. Skarita, F.J. Willeke
    BNL, Upton, Long Island, New York
 
 

NSLS-II is a third-generation light source that is being built at the Brookhaven National Laboratory. The storage ring has 30 double-bend-achromatic cells. Six 3.5-m-long damping wigglers (DW) will be installed in three straight section to lower the emittance. The civil construction of the facility started in June 2009 and major accelerator components, such as magnets and vacuum chambers, have entered production phase. This paper will summarize the physics considerations for the NSLS-II magnet specifications. In particular, we discuss the tuning range required by the lattice flexibility, and the issues which lead to the specification for the higher-order multipoles.

 
WEPEA082 Status of the NSLS-II Injection System Development booster, linac, storage-ring, injection 2672
 
  • T.V. Shaftan, A. Blednykh, W.R. Casey, L.R. Dalesio, R. Faussete, M.J. Ferreira, R.P. Fliller, G.S. Fries, G. Ganetis, W. Guo, R. Heese, H.-C. Hseuh, Y. Hu, P.K. Job, E.D. Johnson, Y. Kawashima, B.N. Kosciuk, S. Kowalski, S. Krinsky, Y. Li, H. Ma, R. Meier, S. Ozaki, D. Padrazo, B. Parker, I. Pinayev, M. Rehak, J. Rose, S. Sharma, O. Singh, P. Singh, J. Skaritka, C.J. Spataro, G.M. Wang, F.J. Willeke, L.-H. Yu
    BNL, Upton, Long Island, New York
 
 

We discuss status and plans of development of the NSLS-II injector. The injector consists of 200 MeV linac, 3-GeV booster, transport lines and injection straight section. The system design is now nearly completed and the injector development is in the procurement phase. The injector commissioning is planned to take place in 2012.

 
WEPEA083 Application of Model Independent Analysis with EPICS-DDS EPICS, booster, controls, optics 2675
 
  • N. Malitsky, I. Pinayev
    BNL, Upton, Long Island, New York
  • R.M. Talman
    CLASSE, Ithaca, New York
  • C. Xiaomeng
    Stony Brook University, Stony Brook
 
 

Model Independent Analysis (MIA) is an essential approach for measuring optical properties of accelerators. In the paper, we evaluate its application in the context of the NSLS-II Light Source storage ring. It is the first application of the new high-level application environment based on the EPICS-DDS middle layer. Using a full-scale virtual accelerator, the paper explores the tolerance of the MIA approach against the different conditions such as measurement noise in the beam position monitors, magnet errors, misalignments, etc.

 
WEPEB022 The NTMAT EPICS-DDS Virtual Accelerator for the Cornell ERL Injector EPICS, controls, simulation, power-supply 2734
 
  • C.M. Gulliford, I.V. Bazarov, J. Dobbins, R.M. Talman
    CLASSE, Ithaca, New York
  • N. Malitsky
    BNL, Upton, Long Island, New York
 
 

Commissioning of the high brightness photoinjector for the Energy Recovery Linac at Cornell University continues. To aid in this process we have developed a 'Virtual Accelerator' application, which provides the beam physicist with an online high-level physics description of the machine. This application combines a linear optics model called Numerical Transfer Matrix (NTMAT), developed at Cornell, and EPICS-DDS, a middle-layer software based on the Experimental Physics and Industrial Control System (EPICS) toolkit and the Data Distribution Service (DDS) data-centric publish/subscribe model. We present the initial results of implementing this new software tool and its deployment in the Cornell ERL injector control room.

 
WEPEB027 Preliminary Operational Experiences of a Bunch-by-bunch Transverse Feedback System at the Australian Synchrotron synchrotron, sextupole, feedback, insertion 2743
 
  • D.J. Peake, R.P. Rassool
    Melbourne
  • M.J. Boland, R.T. Dowd, Y.E. Tan
    ASCo, Clayton, Victoria
 
 

The Australian Synchrotron storage ring has a resistive wall instability in the vertical plane. Presently this instability is being controlled by increasing the vertical chromaticity. However new in-vacuum insertion devices that significantly increase the ring impedance may demand chromatic corrections beyond the capabilities of the sextupole magnets. A transverse bunch-by-bunch feedback system has been commissioned to combat the vertical instability* and provide beam diagnostics**. A high frequency narrow band mode that could not be damped was initial encountered with IVUs at minimum gap preventing the system from being implemented during user beam. Tuning of the bunch fill pattern, the digital filters and mapping out the system response lead to a configuration for user mode operations.


* Spencer, M.J. et. al. EPAC'08, Genoa, Italy
** Peake, D.J. et. al. PAC'09, Vancouver, Cananda

 
WEPEB075 Beam Halo Studies for CTF3 resonance, diagnostics, controls, beam-losses 2872
 
  • S.T. Artikova
    MPI-K, Heidelberg
  • R.B. Fiorito, A.G. Shkvarunets, H.D. Zhang
    UMD, College Park, Maryland
  • C.P. Welsch
    Cockcroft Institute, Warrington, Cheshire
 
 

Beam halo can have severe effects on the performance of high energy accelerators. It reduces the experimental throughput, may lead to noise in the experiments, or even damaging of accelerator components. In order to understand and ideally control the formation and evolution of beam halo, detailed simulation studies are required. In this contribution halo generation mechanisms and the underlying physical principles are first presented, before the particular case of the CLIC Test Facility (CTF3) is discussed in detail. Analytical, numerical and simulation studies are combined to estimate the relevant sources of halo formation and to study halo propagation in the different CTF3 sections.

 
WEPEC002 Titanium Nitride Coating as a Multipactor Suppressor multipactoring, vacuum, electron, target 2887
 
  • W. Kaabi, A. Variola
    LAL, Orsay
  • A. Brinkmann
    DESY, Hamburg
  • G. Keppel, V. Palmieri
    INFN/LNL, Legnaro (PD)
  • I. Montero
    CSIC, Madrid
 
 

LAL-Orsay is developing an important effort on R&D and technology studies on RF power couplers for superconductive cavities. One of the most critical components of those devices is the ceramic RF window that allows the power flux to be injected in the coaxial line. The presence of a dielectric window on a high power RF line has a strong influence on the multipactor phenomena. The most important method to reduce the multipactor is to decrease the secondary emission yield of the ceramic window. Due to its low Secondary electron Emission Yield (SEY), TiN thin film is used as a multipactor suppressor coating on RF ceramic coupler windows. In this frame work, TiN deposition was made by magnetron reactive sputtering. XPS and XRD analysis were performed to control the film composition and stoechiometry. Coating thickness was optimized so that the TiN coating effectively reduces the SEY but does not cause excessive heating, due to ohmic loss. For this purpose, SEY measurements on covered and uncovered TiN Alumina substrates, multipactor level breakdown on TiN coated Cupper substrates and RRR measurements were performed for different deposit thicknesses.

 
WEPEC054 Status of the CLIC RTML Studies emittance, linac, electron, simulation 3013
 
  • F. Stulle, D. Schulte, J. Snuverink
    CERN, Geneva
  • A. Latina
    Fermilab, Batavia
  • S. Molloy
    Royal Holloway, University of London, Surrey
 
 

Over the last months the general layout of the CLIC main beam RTML has stabilized and most important lattices are existing. This allowed us to perform detailed studies of tolerances on magnetic stray fields and on magnet misalignment. Additionally, beam lines could be improved in terms of performance and flexibility. We discuss the overall layout as will be described in the CLIC conceptual design report, highlight the improvements which have been made and show results of tolerance studies.

 
WEPD024 New Scheme of Quasi-Periodic Undulators undulator, radiation, photon, synchrotron 3141
 
  • S. Sasaki
    HSRC, Higashi-Hiroshima
 
 

More than a decade has past after the original quasi-periodic undulator (QPU) was proposed.* Until now, much work has been done to improve the QPU performance. One of the first most productive improvements was to introduce the quasi-periodicity in an electron trajectory by partially changing the field strength in a periodic undulator.** Also, a modification of creation theory of one-dimensional quasi-periodicity gave another degree of freedom to build this type of device.*** As the result, many different types of QPUs have been and will be installed in the synchrotron radiation facilities worldwide.**** In this paper, a new scheme of quasi-periodic undulator that has a different magnetic structure is proposed. This new QPU generates a slightly higher intensity radiation with higher harmonics pattern different from those of previous QPUs. This new scheme of QPU is achieved by introducing orthogonal field in each half-period in order to create additional phase delay of electron beam at certain positions predicted by the theory. We discuss about realistic magnetic configurations as well as possibilities and limitations of new-QPUs.


* Hashimoto, Sasaki, NIM A361, 611 (1995)
** Chavanne, et al, Proc EPAC98, p2213, Diviacco, et al, ibid, p2216
*** Sasaki, et al, Proc EPAC98, p2237
**** Steier, et al, Proc EPAC08, p2311

 
WEPD025 Theoretical Examination of Radiation Spectrum from the Quasi-periodic Undulator radiation, undulator, synchrotron, synchrotron-radiation 3144
 
  • S. Hirata
    Hiroshima University, Faculty of Science, Higashi-Hirosima
  • S. Sasaki
    HSRC, Higashi-Hiroshima
 
 

Different form conventional periodic undulators, the quasi-periodic undulator (QPU) can radiate irrational harmonics instead of rational harmonics. It suits with experiments that need highly monochromatic light after passing through the monochromator. For this reason, the QPU is used in many synchrotron radiation facilities all over the world. Recently, new type QPUs that generate radiation spectra different from those by conventional type QPU were proposed*,**. In principle, the shape of radiation spectrum from a new QPU is determined by magnetic field distribution having different quasi periodic pattern. However, calculated spectra using a realistic magnetic field are often different from those of theoretical expectation. In this paper, a detailed comparative study is conducted to examine why there are these differences, how to correct magnetic field to get predicted spectra that fit to the theory. In addition, a possibility of modifying the basis of theory is investigated. These results, new generation method of new quasi-periodicity, and magnetic field distribution to achieve the best performance are presented at the conference.


* S. Sasaki, Proceedings of PAC09, Vancouver, May, 2009.
** S. Sasaki, Proceedings of 6th Annual Meeting of Particle Accelerator Society of Japan (in Japanese).

 
WEPD057 Linac Energy Management for LCLS klystron, linac, controls, optics 3224
 
  • P. Chu, R.H. Iverson, P. Krejcik, D. Rogind, G.R. White, M. Woodley
    SLAC, Menlo Park, California
 
 

Linac Energy Management (LEM) is a control system program which calculates, and optionally implements, magnet setpoint settings (BDESs) following a change in Energy (such as a change in the number, phase, and amplitude of active klystrons). The change is made relative to those magnets' existing BDES setpoints by a factor encoding the change in energy. LEM is necessary because changes in the number, phase, and amplitude of the active klystrons (the so-called "Klystron complement") change the beam's rigidity, and therefore, to maintain constant optics, one has to change focusing gradients and bend fields. This paper describes the basic process and some of the implementation lessons learned for LEM at the LCLS.

 
WEPD065 Storage Ring Magnet Power Supply System at the PLS-II quadrupole, sextupole, power-supply, septum 3248
 
  • S.-C. Kim, K.R. Kim, S.H. Nam, C.D. Park, Y.G. Son, C.W. Sung
    PAL, Pohang, Kyungbuk
 
 

Lattice of the Storage Ring (SR) is changed from TDB to DBA, and beam energy is enhanced from 2.5 GeV to 3.0 GeV at the Pohang Light Source upgrade (PLS-II). Therefore all magnet specification and number have to change compare with exist PLS SR. At the PLS-II, Magnet Power Supplies (MPS) must be re-designed according to magnet specification of the PLS-II. Newly development MPSs are adopted switching type power conversion technology. High current unipolar MPSs are parallel operation type of unit module buck type power supply, and low current bipolar MPSs are H-bridge type. All MPSs are performed ± 10 ppm output current stability and adopted full digital controller. In this paper, we report on the development and characteristics of the MPS for PLS-II SR.

 
WEPE030 The CLIC BDS Towards the Conceptual Design Report luminosity, alignment, collimation, quadrupole 3419
 
  • R. Tomás, B. Dalena, E. Marin, D. Schulte, G. Zamudio
    CERN, Geneva
  • D. Angal-Kalinin, J.-L. Fernandez-Hernando, F. Jackson
    Cockcroft Institute, Warrington, Cheshire
  • J. Resta-López
    JAI, Oxford
  • A. Seryi
    SLAC, Menlo Park, California
 
 

The CLIC Conceptual Design Report must be ready by 2010. This paper aims at addressing all the critical points of the CLIC BDS to be later implemented in the CDR. This includes risk evaluation and possible solutions to a number of selected points. The smooth and practical transition between the 500 GeV CLIC and the design energy of 3 TeV is also studied.

 
WEPE031 Beam Delivery System Dogleg Design and Integration for the International Linear Collider emittance, dipole, undulator, positron 3422
 
  • J.K. Jones, D. Angal-Kalinin
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

It is proposed to investigate the option of moving the positron source to the end of the main linac as a part of the central integration in the International Linear Collider project. The positron source incorporates an undulator at the end of the main linac and the photons generated in the undulator are transported to the target, located at a distance of around 400m. The dogleg design has been optimised to provide the required transverse off-set at the location of the target and to give minimum emittance growth at 500 GeV. The design of the dogleg and the tolerances on beam tuning as a result of locating this dogleg in the beginning of the beam delivery system are presented.

 
WEPE037 Optimization of Dynamic Aperture of PEP-X Baseline Design sextupole, dynamic-aperture, emittance, injection 3437
 
  • M.-H. Wang, Y. Cai, Y. Nosochkov
    SLAC, Menlo Park, California
 
 

SLAC is developing a long-range plan to transfer the evolving scientific programs at SSRL from the SPEAR3 light source to a much higher performing photon source that would be housed in the 2.2-km PEP-II tunnel*,**. The proposed PEP-X storage ring is one of the possibilities. The goal of the PEP-X design is to develop an optimal light source design with horizontal emittance less than 100 pm at 4.5 GeV and vertical emittance of 8 pm corresponding to the diffraction limit of 1-Å X-ray. The low emittance design requires a lattice with strong focusing leading to high natural chromaticity and therefore to strong sextupoles. The latter cause reduction of dynamic aperture. The horizontal dynamic aperture required at PEP-X injection point is about 10 mm. In order to achieve the desired dynamic aperture, transverse non-linearities of PEP-X are studied. The program LEGO*** is used for particle tracking simulations. The technique of frequency map is used to analyze the nonlinear behavior. The effects of the non-linearities are tried to minimize. The details and results of dynamic aperture optimization are discussed in this paper.


*,** R. Hettel et al., 'IDEAS FOR A FUTURE PEP-X LIGHT SOURCE', EPAC08, 'CONCEPTS FOR THE PEP-X LIGHT SOURCE', PAC09.
*** Y. Cai et al., 'LEGO: A Modular accelerator design code', PAC97, 1997.

 
WEPE043 Study for a Racetrack FFAG based Muon Ring Cooler cavity, kicker, injection, emittance 3446
 
  • A. Sato
    Osaka University, Osaka
 
 

FFAG lattices with racetrack-shape has been studied to cool muon beams. The ring has straight sections with FFAG magnets, which makes enough space to install kicker magnets to inject and extract the muon beam. Wedge absorbers using superfluid helium and RF cavities are installed to the ring. This paper reports progress of the study.

 
WEPE050 Alternative Muon Front-end for the International Design Study (IDS) cavity, proton, acceleration, target 3455
 
  • C.T. Rogers
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • A. Alekou
    Imperial College of Science and Technology, Department of Physics, London
  • M. Martini, G. Prior
    CERN, Geneva
  • D.V. Neuffer
    Fermilab, Batavia
  • D. Stratakis
    BNL, Upton, Long Island, New York
  • C. Y. Yoshikawa
    Muons, Inc, Batavia
  • M.S. Zisman
    LBNL, Berkeley, California
 
 

We discuss alternative designs of the muon capture front end of the Neutrino Factory International Design Study (IDS). In the front end, a proton bunch on a target creates secondary pions that drift into a capture channel, decaying into muons. A sequence of RF cavities forms the resulting muon beams into strings of bunches of differing energies, aligns the bunches to (nearly) equal central energies, and initiates ionization cooling. This design is affected by limitations on accelerating gradients within magnetic fields. The effects of gradient limitations are explored, and mitigation strategies are presented.

 
WEPE051 Muon Cooling Performance in Various Neutrino Factory Cooling Cell Configurations using G4MICE factory, cavity, emittance, betatron 3458
 
  • A. Alekou, J. Pasternak
    Imperial College of Science and Technology, Department of Physics, London
  • C.T. Rogers
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

The Neutrino Factory is a planned particle accelerator complex that will produce an intense, focused neutrino beam, using neutrinos from muon decay. Such high neutrino intensities can only be achieved by reducing the muon beam emittance using an ionization cooling system. The G4MICE software is used to study the performance of various cooling cell configurations. A comparison is drawn between the cooling in the FS2 cells, the baseline Neutrino Factory and doublet cells. The beam dynamics in each of cooling channels are presented. The lattices are compared with respect to the equilibrium emittance, muon transmission, acceptance and evolution of emittance along the channel. Conclusions for a possible optimisation of the future muon cooling channel of the Neutrino Factory are presented.

 
WEPE056 Accelerator and Particle Physics Research for the Next Generation Muon to Electron Conversion Experiment - the PRISM Task Force injection, extraction, kicker, betatron 3473
 
  • J. Pasternak, L.J. Jenner, Y. Uchida
    Imperial College of Science and Technology, Department of Physics, London
  • R.J. Barlow
    UMAN, Manchester
  • K.M. Hock, B.D. Muratori
    Cockcroft Institute, Warrington, Cheshire
  • D.J. Kelliher, S. Machida, C.R. Prior
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • Y. Kuno, A. Sato
    Osaka University, Osaka
  • A. Kurup
    Fermilab, Batavia
  • J.-B. Lagrange, Y. Mori
    KURRI, Osaka
  • M. Lancaster
    UCL, London
  • S.A. Martin
    FZJ, Jülich
  • C. Ohmori
    KEK/JAEA, Ibaraki-Ken
  • J. Pasternak
    STFC/RAL, Chilton, Didcot, Oxon
  • S.L. Smith
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • H. Witte, T. Yokoi
    JAI, Oxford
 
 

The next generation of lepton flavour violation experiments will use high intensity and high quality muon beams. Such beams can be produced by sending a short proton pulse to the pion production target, capturing pions and performing RF phase rotation on the resulting muon beam in an FFAG ring, which was proposed for the PRISM project. A PRISM task force was created to address the accelerator and detector issues that need to be solved in order to realise the PRISM experiment. The parameters of the initial proton beam required and the PRISM experiment are reviewed. Alternative designs of the PRISM FFAG ring are presented and compared with the reference design. The ring injection/extraction system, matching with the solenoid channel and progress on the ring's main hardware systems like RF and kicker magnet are discussed. The activity on the simulation of a high sensitivity experiment and the impact on physics reach is described. The progress and future directions of the study are presented in this paper.

 
WEPE057 Injection/Extraction System of the Muon FFAG for the Neutrino Factory kicker, extraction, injection, septum 3476
 
  • J. Pasternak, M. Aslaninejad
    Imperial College of Science and Technology, Department of Physics, London
  • J.S. Berg
    BNL, Upton, Long Island, New York
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • J. Pasternak
    STFC/RAL, Chilton, Didcot, Oxon
  • H. Witte
    JAI, Oxford
 
 

Nonscaling FFAG is required for the muon acceleration in the Neutrino Factory, which baseline design is under investigation in the International Design Study (IDS-NF). In order to inject/extract the muon beam with a very large emittance, several strong kickers with a very large aperture are required distributed in many lattice cells. Once the sufficient orbit separation is obtained by the kickers, the final degree of separation from the lattice is made by the septum, which needs to be superconducting. The geometry of the symmetric solutions allowing to inject/extract both signs of muons is presented. The preliminary design of the kicker and septum magnets is given.

 
WEPE061 Measurements of Muon Beam Properties in MICE emittance, factory, optics, solenoid 3482
 
  • M.A. Rayner, J.H. Cobb
    OXFORDphysics, Oxford, Oxon
 
 

The Muon Ionization Cooling Experiment is one lattice section of a cooling channel suitable for conditioning the muon beam at the front end of a Neutrino Factory or Muon Collider. Scintillating fibre spectrometers and 50 ps resolution timing detectors provide the unprecedented opportunity to measure the initial and final six-dimensional phase space vectors of individual muons. The capability of MICE to study the evolution of muon beams through a solenoidal lattice will be described.

 
WEPE072 Incorporating RF into a Muon Helical Cooling Channel cavity, solenoid, quadrupole, collider 3509
 
  • S.A. Kahn, G. Flanagan, R.P. Johnson, M.L. Neubauer
    Muons, Inc, Batavia
  • V.S. Kashikhin, M.L. Lopes, K. Yonehara, M. Yu, A.V. Zlobin
    Fermilab, Batavia
 
 

A helical cooling channel (HCC) consisting of a pressurized gas absorber imbedded in a magnetic channel that provides solenoidal, helical dipole and helical quadrupole fields has shown considerable promise in providing six-dimensional cooling for muon beams. The energy lost by muons traversing the gas absorber needs to be replaced by inserting RF cavities into the HCC lattice. Replacing the substantial muon energy losses using RF cavities with reasonable gradients will require a significant fraction of the channel length be devoted to RF. However to provide the maximum phase space cooling and minimum muon losses, the HCC should have a short period and length. In this paper we examine an approach where each HCC cell has an RF cavity imbedded in the aperture with the magnetic coils are split allowing for half of the cell length to be available for the RF coupler and other services.

 
WEPE080 Six-Dimensional Cooling Lattice Studies for the Muon Collider cavity, emittance, simulation, collider 3533
 
  • P. Snopok, G.G. Hanson
    UCR, Riverside, California
 
 

A significant reduction in the six-dimensional emittance of the initial beam is required in any proposed Muon Collider scheme. Two lattices based on the original RFOFO ring design representing different stages of cooling are considered. One is the so-called open cavity lattice addressing the problem of the 201.25 MHz RF cavities running in a magnetic field, the other one is the 805 MHz RF lattice that is used for smaller emittances. The details of the acceptance analysis and tracking studies of both channels are presented and compared to the independent ICOOL implementation.

 
WEPE081 Wedge Absorber Design for the Muon Ionisation Cooling Experiment emittance, simulation, scattering, cavity 3536
 
  • P. Snopok, L. Coney
    UCR, Riverside, California
  • A. Jansson
    Fermilab, Batavia
  • C.T. Rogers
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

In the Muon Ionization Cooling Experiment (MICE), muons are cooled by ionization cooling. Muons are passed through material, reducing the total momentum of the beam. This results in a decrease in transverse emittance and a slight increase in longitudinal emittance, but overall reduction of 6D beam emittance. In emittance exchange, a dispersive beam is passed through wedge-shaped absorbers. Muons with higher energy pass through more material, resulting in a reduction in longitudinal and transverse emittance. Emittance exchange is a vital technology for a Muon Collider and may be of use for a Neutrino Factory. Two ways to demonstrate emittance exchange in the straight solenoidal lattice of MICE are discussed. One is to let a muon beam pass through a wedge shaped absorber; the input beam distribution must be carefully selected to accommodate chromatic aberrations in the solenoid lattice. Another approach is to use the input beam for MICE without beam selection. In this case no polynomial weighting is involved; however, a more sophisticated shape of the absorber is required to reduce longitudinal emittance.

 
WEPE084 Muon Acceleration with RLA and Non-scaling FFAG Arcs linac, optics, sextupole, quadrupole 3539
 
  • V.S. Morozov
    ODU, Norfolk, Virginia
  • S.A. Bogacz
    JLAB, Newport News, Virginia
  • D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

Recirculating linear accelerators (RLA) are the most likely means to achieve the rapid acceleration of short-lived muons to multi-GeV energies required for Neutrino Factories and TeV energies required for Muon Colliders. In the work described here, a novel arc optics based on a Non Scaling Fixed Field Alternating Gradient (NS-FFAG) lattice is developed, which would provide sufficient momentum acceptance to allow multiple passes (two or more consecutive energies) to be transported in one string of magnets. We present a combination of the non-scaling NS-FFAG RLA placed in a straight section. Orbit offsets of different energy muons are kept small in the NS-FFAG arcs during multiple passes. The NS-FFAG, made of densely packed FODO cells, allows momentum acceptance of dp/p=±60%. This solution would reduce overall cost and simplify the operation. Difference in a muon path length for corresponding energies is corrected with a chicane. We will also discuss technical requirements to allow the maximum number of passes by using an adjustable path length to accurately control the returned beam phase to synchronize with the RF.

 
WEPE086 A Low Emittance Lattice for the ILC 3 km Damping Ring damping, wiggler, emittance, dynamic-aperture 3545
 
  • S. Guiducci, M.E. Biagini
    INFN/LNF, Frascati (Roma)
 
 

A new baseline parameter set has been proposed for the ILC with a reduction by a factor 2 in the number of bunches. This option will allow for a corresponding factor 2 decrease in the Damping Ring circumference, with significant cost savings. A low emittance lattice for a 3.2 km long damping ring has been designed, with the same racetrack layout of the present reference 6.4 km long lattice and similar straight sections. The technical work done for the longer ring can be easily applied to the shorter one. The lattice is based on an arc cell design adopted for the SuperB collider and allows some flexibility in tuning emittance and momentum compaction.

 
WEPE088 A New Design for ILC 3.2 km Damping Ring Based on FODO Cell damping, wiggler, dipole, quadrupole 3551
 
  • D. Wang, J. Gao, Y. Wang
    IHEP Beijing, Beijing
 
 

In this paper, we made a new design for ILC 3.2 km damping ring with 2 arcs based on FODO cell and 2 straight sections which are nearly the same as the new version of the 6.4 km ring DCO4. This new lattice uses less dipoles and quadrupoles than the present SuperB like lattice and has an adequate aperture for the large injected emittance of the positron beam. The work of lattice design and DA optimization will be presented in detail.

 
WEPE090 Intra-Beam Scattering in the CLIC Damping Rings emittance, damping, simulation, radiation 3557
 
  • A. Vivoli, M. Martini
    CERN, Geneva
 
 

The CLIC 3 TeV nominal design requires very low emittance of the electron and positron beams to be reached in the damping rings. Due to low energy and to relatively high bunch charge and ultra-low emittance, Intra-Beam Scattering (IBS) effect is very strong and an accurate calculation is needed to check if the required emittance is effectively reached. For this reason it is being developed at CERN a new Software for IBS and Radiation Effects (SIRE), which simulates the evolution of the beam particle distribution in the damping rings, taking into account radiation damping, IBS and quantum excitation. In this paper we present the results of our simulations performed with SIRE on the current lattice of the CLIC damping rings.

 
WEPE095 Impedance and Single-bunch Instabilities in the ILC Damping Ring wakefield, insertion, damping, vacuum 3572
 
  • M. Korostelev, O.B. Malyshev, A. Wolski
    Cockcroft Institute, Warrington, Cheshire
  • N.A. Collomb, J.M. Lucas, S. Postlethwaite
    STFC/DL, Daresbury, Warrington, Cheshire
  • A.J.P. Thorley
    The University of Liverpool, Liverpool
 
 

The longitudinal wake fields have been calculated by using 3D code, CST Particle Studio, for a number of different vacuum chamber components of the 6.4 km ILC damping ring design. Based on the results, studies of bunch lengthening and single-bunch instabilities have been carried out. Bunch lengthening from a particle tracking code are compared with results from numerical solution of the Haissinski equation. The tracking code is used to predict the threshold for single-bunch instabilities.

 
WEPE096 DCO4 Lattice Design for 6.4 km ILC Damping Rings extraction, injection, positron, damping 3575
 
  • M. Korostelev, A. Wolski
    Cockcroft Institute, Warrington, Cheshire
 
 

A new lattice design for the ILC damping ring has been developed since the beginning of 2008 as a lower cost alternative to the previous OCS6 design. The lattices for the electron and positron damping rings are identical, and are designed to provide an intense, 5 GeV beam with low emittance at extraction. The latest design, presented in this paper, provides sufficient dynamic aperture for the large positron beam at injection. The lattice also meets the engineering requirements for arrangement of the positron ring directly above the electron ring in the same tunnel, using common girders for the magnets in the two rings, but with the beams circulating in opposite directions.

 
THXMH01 Commissioning of the EMMA Non-Scaling FFAG injection, acceleration, resonance, emittance 3593
 
  • T.R. Edgecock
    STFC/RAL, Chilton, Didcot, Oxon
 
 

EMMA is the world's first non-scaling fixed field alternating gradient accelerator and is being constructed at the STFC Daresbury Laboratory. Experience from the initial commissioning phases (from early 2010) will be reported and lessons for future machines of a similar type will be discussed. The present experimental status and future plans will also be reported.

 

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THOAMH01 Recirculating Linear Accelerators for Future Muon Facilities linac, optics, focusing, acceleration 3602
 
  • S.A. Bogacz
    JLAB, Newport News, Virginia
  • K.B. Beard, R.P. Johnson
    Muons, Inc, Batavia
 
 

Neutrino Factories and Muon Colliders require rapid acceleration of short-lived muons to multi-GeV and TeV energies. A Recirculating Linear Accelerator (RLA) that uses superconducting RF structures can provide exceptionally fast and economical acceleration to the extent that the focusing range of the RLA quadrupoles allows each muon to pass several times through each high-gradient cavity. A new concept of rapidly changing the strength of the RLA focusing quadrupoles as the muons gain energy is being developed to increase the number of passes that each muon will make in the RF cavities, leading to greater cost effectiveness. We discuss the optics and technical requirements for RLA designs, using RF cavities capable of simultaneous acceleration of both μ+ and μ- species, with pulsed Linac quadrupoles and arc magnets to allow the maximum number of passes. The design will include the optics for the multi-pass linac and droplet-shaped return arcs.

 

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THOBRA02 Suppression of Transverse Instabilities by Chromaticity Modulation damping, synchrotron, betatron, feedback 3647
 
  • T. Nakamura, N. Kumagai, S. Matsui, H. Ohkuma, T. Ohshima, H. Takebe
    JASRI/SPring-8, Hyogo-ken
  • A. Ando, S. Hashimoto, Y. Shoji
    NewSUBARU/SPring-8, Laboratory of Advanced Science and Technology for Industry (LASTI), Hyogo
  • K. Kumagai
    RIKEN Nishina Center, Wako
 
 

Transverse beam instabilities were suppressed with chromaticity modulation (CM)* in the electron storage ring, New SUBARU. The horizontal and vertical betatron tune spread inside a bunch were introduced by CM with synchrotron oscillation frequency driven by an AC sextuple magnet**, to obtain Landau damping of the coherent bunch motion. The tune spread in a bunch is usually introduced by octupole field, however, its high nonlinearity reduces the dynamic aperture. And usual feedback against instabilities work only on m=0 mode and it is not easy to be applied to hadron synchrotrons because of their varying revolution period. The CM scheme has not such disadvantages. The damping time of coherent motion excited by external kick was measured and was found as less than 1ms, one order faster than that without CM. To observe the effect on instabilities, we intentionally tuned an HOM in a cavity to excite a horizontal multi-bunch instability. The instability peak in the spectrum of the beam motion was vanished with CM turned on and the instability was suppressed. We also observed the increase of the threshold current of the vertical single-bunch mode-coupling instability by factor 3 with CM.


* T. Nakamura, Proc. of PAC'95, p.3100 (1995).
** T. Nakamura, et al., Appl. Superconduct., IEEE Trans. Vol. 18, p.326 (2008).

 

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THPEB004 Slow Extraction from the Superconducting Synchrotron SIS300 at FAIR: Lattice Optimization and Compensation of Field Errors sextupole, dipole, extraction, resonance 3882
 
  • A. Saa Hernandez, H. Mueller, N. Pyka, P.J. Spiller
    GSI, Darmstadt
  • U. Ratzinger
    IAP, Frankfurt am Main
 
 

With the ability to accelerate heavy ions up to an energy of 32 GeV/u, the SIS300 superconducting (sc) synchrotron is a central part of the new FAIR facility at GSI-Darmstadt. SIS300 will provide beams with a 20-fold increase in energy and, by means of a stretcher mode or a fast ramped mode (1 T/s), 100-10000 times higher average intensity. The beam from SIS300 will be extracted towards the experiments using resonant slow extraction, thus SIS300 becomes the first superconducting synchrotron worldwide with this feature. Coupling and persistent currents are the main practical limitation for operation of sc magnets at high ramping rates and long slow extraction plateaus. The effect of the persistent currents, which are time dependent and depend as well on the magnet's history, is especially critical for slow extraction at low energies. These effects determine the tolerances on magnetic components. In order to address this issue, detailed simulations of beam dynamics at slow extraction have been performed. In particular, the optimization of the lattice and its optical parameters for a low-loss extraction in the presence of steady and time-dependent field components will be presented.

 
THPEB057 Design of Photonic Crystal Klystrons klystron, cavity, electron, simulation 4002
 
  • Y. Xu
    Lancaster University, Lancaster
  • R. Seviour
    Cockcroft Institute, Lancaster University, Lancaster
 
 

2D Photonic crystals (PC) with defects can act as standing-wave resonators, which offer benefit of high mode selectivity for building novel RF sources. We introduce our work on designing two-cavity single-beam and multi-beam klystrons using triangular lattice metallic PCs. We present the cold test results of the stub-coupled single-beam structure, which show that at resonance a very low reflection can be obtained, and the waves are well confined. We also present bead-pull measurement results of field strengths in the defect, using modified perturbation equation for small unit dielectric cylinder, which are in very good agreement to numerical results. A 6-beam klystron cavity is designed as a 6-coupled-defect structure with a central stub, which only couples to the in-phase mode at the lowest frequency. Finally, we present a feasibility discussion of using this multi-defect PC structure to construct an integrated klystron-accelerator cavity, along with numerical results showing a peak acceleration field of 22MV/m can be achieved.

 
THPEC013 Compact Couplers for Photonic Crystal Laser-driven Accelerator Structures coupling, simulation, laser, acceleration 4077
 
  • B.M. Cowan, M.C. Lin, B.T. Schwartz
    Tech-X, Boulder, Colorado
  • R.L. Byer, C. McGuinness
    Stanford University, Stanford, California
  • E.R. Colby, R.J. England, R.J. Noble, J.E. Spencer
    SLAC, Menlo Park, California
 
 

Photonic crystal waveguides are promising candidates for laser-driven accelerator structures because of their ability to confine a speed-of-light mode in an all-dielectric structure. Because of the difference between the group velocity of the waveguide mode and the particle bunch velocity, fields must be coupled into the accelerating waveguide at frequent intervals. Therefore efficient, compact couplers are critical to overall accelerator efficiency. We present designs and simulations of high-efficiency coupling to the accelerating mode in a three-dimensional photonic crystal waveguide from a waveguide adjoining it at 90 degrees. We discuss details of the computation, including an optimization routine to modify the geometric parameters of the coupler for maximum efficiency, the resulting transmission, and estimates of the fabrication tolerance for these devices. We include some background on the accelerator structure and photonic crystal-based optical acceleration in general.

 
THPD022 FFAG Tracking with Cyclotron Codes cyclotron, TRIUMF, proton, ion 4319
 
  • M.K. Craddock
    UBC & TRIUMF, Vancouver, British Columbia
  • Y.-N. Rao
    TRIUMF, Vancouver
 
 

This paper describes tracking studies of non-scaling (NS) FFAGs using cyclotron codes in place of the more conventional lumped-element synchrotron codes. The equilibrium orbit code CYCLOPS determines orbits, tunes and period at fixed energies, while the general orbit code GOBLIN tracks a representative bunch of particles through the acceleration process. Results will be presented for the EMMA linear NS-FFAG under construction at Daresbury (10-20 MeV electrons), and for two non-linear NS-FFAG designs: Rees's isochronous IFFAG (8-20 GeV muons) and Johnstone's design for ADSR (250-1000 MeV protons). Our results are compared with those obtained using lumped-element codes. In the case of EMMA, results are presented for both the measured and design fields.

 
THPD024 Recent Developments On The EMMA On-line Commissioning Software injection, EPICS, septum, extraction 4325
 
  • F. Méot
    CEA, Gif-sur-Yvette
  • J.S. Berg
    BNL, Upton, Long Island, New York
  • Y. Giboudot
    Brunel University, Middlesex
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • B.J.A. Shepherd
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • S.C. Tygier
    UMAN, Manchester
 
 

The EMMA (Electron Model for Many Applications) FFAG experiment at Daresbury will involve on-line modeling (a ‘‘Virtual EMMA'') based on stepwise ray-tracing methods. Various aspects of the code of concern and of its interfacing to real world - machine and users - are addressed.

 
THPD026 Beam Optics and Magnet Design of Helium Ion FFAG Accelerator ion, focusing, injection, simulation 4331
 
  • H.L. Luo, H. Hao, X.Q. Wang, Y.C. Xu
    USTC/NSRL, Hefei, Anhui
 
 

Fixed-Field Alternating Gradient (FFAG) accelerator accelerates in smaller costs heavy-ion with higher beam current than conventional circular accelerator, which could be more useful for the study of radioactive material. In this paper, the periodic focusing structure model of a Helium ion FFAG with a few MeV energy, which is contributed to study the impact of Helium embitterment on fusion reactor envelope material is proposed. A large-aperture magnet for Helium ion FFAG synchrotron is designed by using a 3D magnetic field simulation code OPERA-3D. The linear and nonlinear beam dynamics is studied through tracking the particle in the magnetic field generated by OPERA-3D.

 
THPD027 Orbit Correction in a non-scaling FFAG closed-orbit, resonance, injection, quadrupole 4334
 
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • S.L. Sheehy
    JAI, Oxford
 
 

EMMA - the Electron Model of Many Applications - is to be built at the STFC Daresbury Laboratory in the UK and will be the first non-scaling FFAG ever constructed. The purpose of EMMA is to study beam dynamics in such an accelerator. The EMMA orbit correction scheme must deal with two characteristics of a non-scaling FFAG: i.e. the lack of a well defined reference orbit and the variation with momentum of the phase advance between lattice elements. In this study we present a novel orbit correction scheme that avoids the former problem by instead aiming to maximise both the symmetry of the orbit and the physical aperture of the beam. The latter problem is dealt with by optimising the corrector strengths over the energy range.

 
THPD042 Dispersion Engineering and Disorder in Photonic Crystals for Accelerator Applications dipole, HOM, accelerating-gradient, wakefield 4375
 
  • R. Seviour
    Lancaster University, Lancaster
 
 

The possibility of achieving higher accelerating gradients at higher frequencies with the reduction of the effect of HOMs, compared to conventional accelerating structures, is increasing interest in the possible use of Photonic Crystals (PC) for accelerator applications. In this paper we analyze how the properties of the lattice of a PC resonator can be engineered to give a specific band structure, and how by tailoring the properties of the lattice specific EM modes can either be confined or moved into the propagation band of the PC. We further go on to discuss the role of disorder in achieving mode confinement and how this can be used to optimize both the Q and the accelerating gradient of a PC based accelerating structure. We also examine the use of high disorder to give rise to Anderson Localization, which gives rise to exponential localization of an EM mode. Discussing the difference between the extended Bloch wave, which extends over the entire PC, and the Anderson localized mode.

 
THPD063 Design and High Power Test of Photonic Bandgap Structures for Accelerator Applications HOM, damping, cavity, vacuum 4428
 
  • B.J. Munroe, R.A. Marsh, M.A. Shapiro, R.J. Temkin
    MIT/PSFC, Cambridge, Massachusetts
 
 

Photonic bandgap (PBG) structures show promising results for use in future collider applications. Both acceleration and wakefield damping have been demonstrated experimentally. The breakdown performance of a single cell PBG structure was tested at X-band at SLAC and found to have significant contributions from magnetic field effects. A new structure has been designed at 17.1 GHz to be tested at MIT to investigate the scaling of these and other breakdown effects with frequency. The 17.1 GHz structure will also use the open nature of the PBG lattice to greatly improve the breakdown diagnostics. Finally, a novel PBG structure has been designed for testing at SLAC using elliptical inner rods. This design significantly reduces the pulsed heating in the structure and should therefore improve the breakdown performance.

 
THPD066 Observation of Wakefields in a Beam-Driven Photonic Band Gap Accelerating Structure dipole, wakefield, HOM, electron 4431
 
  • C.-J. Jing
    Euclid TechLabs, LLC, Solon, Ohio
  • S.P. Antipov, M.E. Conde, W. Gai, F. Gao, J.G. Power, Z.M. Yusof
    ANL, Argonne
  • H. Chen, C.-X. Tang, S.X. Zheng
    TUB, Beijing
  • P. Xu
    Tsinghua University, Beijing
 
 

Wakefield excitation has been experimentally studied in a 3-cell X-band standing wave Photonic Band Gap (PBG) accelerating structure. Major monopole (TM01- and TM02-like) and dipole (TM11- and TM12-like) modes were indentified and characterized by precisely controlling the position of beam injection. The quality factor Q of the dipole modes was measured to be ~10 times smaller than that of the accelerating mode. A charge sweep, up to 80 nC, has been performed, equivalent to ~30 MV/m accelerating field on axis. A variable delay low charge witness bunch following a high charge drive bunch was used to calibrate the gradient in the PBG structure by measuring its maximum energy gain and loss. Experimental results agree well with numerical simulations.

 
THPD090 Design of Modified Lattice of Long Straight Section in the SPring-8 Storage Ring sextupole, betatron, dynamic-aperture, undulator 4497
 
  • K. Soutome, K. Fukami, M. Oishi, Y. Okayasu, J. Schimizu, Y. Shimosaki, M. Shoji, M. Takao, H. Yonehara
    JASRI/SPring-8, Hyogo-ken
 
 

A set of three in-vacuum undulators is going to be installed in one of four long straight sections of the SPring-8 storage ring. In order to make the undulator gap as narrow as possible, we plan to divide this long straight section into three sub-sections and install quadrupole magnets between these sub-sections to lower the vertical betatron function. In the modified lattice, however, the symmetry of the ring is lowered and in general it becomes difficult to keep a sufficient dynamic aperture for on- and off-momentum electrons. The long straight sections were originally introduced in the year 2000 and at that time we developed a method of "quasi-transparent matching of sextupole fields" where two key concepts of betatron phase matching and local chromaticity correction were combined to obtain a sufficient dynamic aperture and momentum acceptance. Then, in the year 2007 "counter-sextupole magnets" were further installed to cancel the effect due to non-linear kick by sextupole magnets used for local chromaticity correction. In designing the new lattice with a modified long straight section, we followed the same line and could recover the dynamic aperture and momentum acceptance.

 
THPD092 Applications of Advanced scaling FFAG Accelerator insertion, target, proton, closed-orbit 4503
 
  • J.-B. Lagrange, Y. Ishi, Y. Kuriyama, Y. Mori, K. Okabe, T. Planche, T. Uesugi, E. Yamakawa
    KURRI, Osaka
 
 

Until today, scaling FFAG accelerator were only designed in a ring shape. But a new criteria of the magnetic field configuration satisfying the scaling condition even for straight FFAG beam line has been recently found. Moreover, combining different types of cells can be used to imagine new lattices. Various applications using these recent developments are here examined: inprovements of the PRISM project and the ERIT project, and a zero-chromatic carbon gantry concept are presented.

 
THPD093 New Approaches to Muon Acceleration with Zero-chromatic FFAGS acceleration, cavity, emittance, factory 4506
 
  • T. Planche, Y. Ishi, Y. Kuriyama, J.-B. Lagrange, Y. Mori, K. Okabe, T. Uesugi, E. Yamakawa
    KURRI, Osaka
 
 

The acceleration of intense muon beams up to 25 GeV is the challenge of the international design work for a future neutrino factory. The present baseline scenario for muon acceleration is based on linacs, recirculating linear accelerators (RLAs) and non-scaling fixed field alternating gradient (FFAG) rings. However RLAs are one of the most cost driving part. Two new approaches to use zero-chromatic FFAG instead of RLA have been proposed. Detailed lattices parameters and 6D tracking results are presented.

 
THPE001 Low Emittance Lattice Optimization Using Multiobjective Genetic Algorithm emittance, storage-ring, quadrupole, optics 4515
 
  • W.W. Gao, W. Li, L. Wang
    USTC/NSRL, Hefei, Anhui
 
 

Low emittance is a desirable performance for high brightness synchrotron light source and damping ring. The work presented in this paper demonstrates that the lattice of a given electron storage ring, which has fixed circumference and magnet layout, can be optimized to obtain low emittance by using MOGA (Multi-objective Genetic Algorithm). Both dispersion-free and non-dispersion-free lattices of HLS (Hefei Light Source) upgrade project are computed as an illustration. Simulation result shows that this method is fast and straightforward.

 
THPE005 Beam Polarization Theory and its Application to HLS Storage Ring polarization, electron, radiation, resonance 4518
 
  • J.Q. Lan, B. Sun, Y.C. Sun, H. Xu
    USTC/NSRL, Hefei, Anhui
 
 

A brief, but clear, review of beam polarization theory is given in the paper. Particularly, the algorithm of spin linear transfer matrix (SLIM) is applied to remark the situation of beam in storage ring, specific to HLS (Hefei Light Source). Theoretical analysis indicates that the beam in HLS, working at 800MeV and 2.58/3.58 transverse tunes, could keep away from a variety of spin resonances, and should be able to build up high polarization.

 
THPE007 The Upgrade of the Hefei Light Source (HLS) Transport Line injection, emittance, dipole, storage-ring 4524
 
  • S.C. Zhang, W. Fan, G. Feng, W.W. Gao, W. Li, L. Wang, H. Xu
    USTC/NSRL, Hefei, Anhui
 
 

To enhance the performance of Hefei Light Source, an upgrade project is undergoing. The magnet lattice of storage ring will be reconstructed with 4 DBA cells, whose advantages are lower beam emittance and more straight section available for insertion devices. In order to assure smooth beam accumulation process under new low emittance lattice, the injector, which is composed of electron linac and beam transfer line, would be updated. The detail of upgrading Hefei Light Source transport line will be described in this paper. It include the upgrading of lattice, the orbit control of beam transfer line and others. It is hopeful to realize a high transfer efficiency and high injection efficiency for new lower beam emittance storage ring.

 
THPE008 Issues on Beam Dynamics in PLS-II emittance, dynamic-aperture, insertion, insertion-device 4527
 
  • J.G. Hwang, S.W. Jang, E.-S. Kim
    Kyungpook National University, Daegu
 
 

Pohang Light Source-Ⅱ (PLS-Ⅱ) is an upgrade project of the existing 2.5 GeV PLS. The circumference, beam current and energy of PLS-Ⅱ storage ring are 281.82 m, 400 mA and 3 GeV, respectively. The upgrade project has many issues on beam dynamics. We investigated lattice optimization such as lattice corrections, dynamic aperture, selection of optimized tune & emittance and effects of insertion devices. MAD, SAD and Elegant have been used to the lattice optimization. We investigated the effects of machine errors and 20 IDs to the dynamic aperture. PLS-Ⅱ lattice include twenty insertion devices and their effects on the beam dynamics are investigated. We also investigate possibility to reduce the emittance by increasing horizontal betatron tune and adjusting the dispersion by using of MAD, SAD and Elegant and also examined the required strengths of sextupoles for the various emittances.

 
THPE014 Round Beam Lattice Correction using Response Matrix at VEPP-2000 closed-orbit, solenoid, dipole, quadrupole 4542
 
  • A.L. Romanov, D.E. Berkaev, I. Koop, A.N. Kyrpotin, E. Perevedentsev, Yu. A. Rogovsky, P.Yu. Shatunov, D.B. Shwartz
    BINP SB RAS, Novosibirsk
 
 

Lattice correction based on orbit responses to dipole correctors and orbit correction based on orbit responses to field gradient variations in quads were successfully implemented on VEPP-2000 [*] for the flat-beam lattice. The round-beam lattice involves strong coupling of vertical and horizontal motions that require a full-coupling analysis in the orbit response technique. Programs used were modified to treat this task. Also, automation and speed enhancements were done that enable a routine use of this technique at VEPP-2000. New experimental results from VEPP-2000 are presented.


* Yu.M.Shatunov et al. Project of a New Electron-Positron Collider VEPP-2000, in: Proc. 7th European Particle Accelerator Conf. (EPAC 2000), Vienna, Austria, 439-441

 
THPE020 Scenarios for the ATF2 Ultra-Low Betas Proposal emittance, quadrupole, wiggler, multipole 4554
 
  • E. Marin, R. Tomás
    CERN, Geneva
  • P. Bambade
    LAL, Orsay
  • S. Kuroda, T. Okugi, T. Tauchi, N. Terunuma, J. Urakawa
    KEK, Ibaraki
  • B. Parker
    BNL, Upton, Long Island, New York
  • A. Seryi, G.R. White, M. Woodley
    SLAC, Menlo Park, California
 
 

The current ATF2 Ultra-Low beta proposal was designed to achieve 20nm vertical IP beam size without considering the multipolar components of the FD magnets. In this paper we describe different scenarios that avoid the detrimental effect of these multipolar errors in the FD. The simplest approach consists in modifying the optics but other solutions are studied as the introduction of new higher order magnets or the replacement of the FD with SC technology. The practical aspects of such an upgrade are the tuning performance and the compatibility with existing devices and instrumentation. These are fully addressed in the paper.

 
THPE021 Comparison of PS2 Lattices with Different Geometries quadrupole, resonance, dynamic-aperture, optics 4557
 
  • Y. Papaphilippou, W. Bartmann, H. Bartosik, M. Benedikt, B. Goddard, A. Lachaize
    CERN, Geneva
  • Y. Senichev
    FZJ, Jülich
 
 

The PS2 ring is designed with negative momentum compaction arc cells and doublet straights. In this paper, different lattice geometries are considered. In particular, a two-fold symmetric lattice with dispersion suppressors and a 3-fold symmetric one with resonant arc cells are compared with respect to their optics properties, and ability to satisfy space and magnet constraints. The tuning flexibility of rings based on these two options is presented. Finally, the impact of different geometries on resonance excitation and dynamic aperture is evaluated.

 
THPE022 Linear Optimization and Tunability of the PS2 Lattice quadrupole, optics, injection, vacuum 4560
 
  • H. Bartosik, W. Bartmann, M. Benedikt, B. Goddard, Y. Papaphilippou
    CERN, Geneva
 
 

The PS2 lattice, based on Negative Momentum Compaction (NMC) arc cells is being optimized in order to accommodate a new all-doublet long-straight section (LSS) design. Apart from smoothing the optics and enabling different tuning solutions for H- injection, the optimization focuses on increasing the available magnet-to-magnet drift space and reducing the quadrupole types and strengths. The variation of lattice parameters for a wide range of working points is presented.

 
THPE023 Non-Linear Analysis of the PS2 Negative Momentum Compaction Lattice sextupole, dynamic-aperture, dipole, quadrupole 4563
 
  • H. Bartosik, M. Benedikt, Y. Papaphilippou
    CERN, Geneva
 
 

This paper describes a detailed analysis of various non-linear effects of the nominal Negative Momentum Compaction lattice for PS2. Chromaticity and orbit correction schemes together with dynamic aperture studies are presented. The impact of magnet errors is being assessed and tolerances are evaluated. Frequency and diffusion maps are produced and, combined with non-linear driving terms analysis, are used for working point optimization.

 
THPE030 Double Mini-Betay Optics for TPS Storage Ring emittance, coupling, multipole, dynamic-aperture 4581
 
  • M.-S. Chiu, H.-P. Chang, H.C. Chao, C.-C. Kuo, H.-J. Tsai, C.H. Yang
    NSRRC, Hsinchu
 
 

To evaluate the feasibility for installing two insertion devices in the long straight sections (12 m long) of the TPS storage ring, two different kinds of the double mini-betay optics (symmetric and asymmetric configurations) were proposed to fulfill this purpose. In the symmetric case a quadrupole triplet is located at the center of the long straight, while in the asymmetric case a quadrupole doublet is used. The effects on the beam dynamics, such as the dynamic aperture, injection efficiency, and lifetime, etc., are presented.

 
THPE032 Calculation of Coupled Lattice Functions from Turn-by-turn Trajectory Data in Storage Rings betatron, quadrupole, coupling, optics 4587
 
  • A. Wolski, M. Korostelev, K.G. Panagiotidis
    The University of Liverpool, Liverpool
 
 

BPMs capable of high resolution turn-by-turn bunch position measurements are becoming increasingly widely used in electron storage rings. Analysis of the data from a set of such BPMs following the excitation of a coherent betatron oscillation can yield useful information for tuning the optics and improving machine performance. This approach to optics measurement has the benefits that the data collection is very fast, and analysis can be local, so that application is as easy for a large ring as for a small one. Here, we describe a technique for using turn-by-turn BPM data to determine lattice functions that describe the local coupling in a storage ring; this may be helpful, for example, for achieving low vertical emittance. We discuss the principles of the technique, give some examples, and discuss possible limitations arising from BPM gain and coupling errors.

 
THPE034 A Non-Scaling FFAG Gantry Design for the PAMELA Project controls, betatron, beam-transport, closed-orbit 4593
 
  • R.J.L. Fenning, A. Khan
    Brunel University, Middlesex
  • T.R. Edgecock
    STFC/RAL, Chilton, Didcot, Oxon
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

A gantry is required for the PAMELA project using non-scaling Fixed Field Alternating Gradient (NS-FFAG) magnets. The NS-FFAG principle offers the possibility of a gantry much smaller, lighter and cheaper than conventional designs, with the added ability to accept a wide range of fast changing energies. This paper will build on previous work to investigate a design which could be used for the PAMELA project.

 
THPE036 Tune Measurement in Non Scaling FFAG EMMA with Model Independent Analysis betatron, simulation, quadrupole, kicker 4596
 
  • Y. Giboudot
    Brunel University, Middlesex
  • I. Kirkman, A. Wolski
    The University of Liverpool, Liverpool
 
 

The Non Scaling Fixed Field Alternating Gradient (NS-FFAG) EMMA accelerator has a purely linear lattice and thus allows important tune variation. The crossing of resonances during acceleration is a key characteristic of the beam dynamics. An accurate measurement of the tune is therefore mandatory. However commonly used measurement techniques requires the beam to perform an important number of turns in the machine. Simulations have shown that fast decoherence of the beam requires the study of another measurement technique. The model independent analysis (MIA) has been investigated. The singular value decomposition (SVD) of a matrix composed of simulated BPMs reading of various bunches trajectories gives a description of the optics function at each Beam Position Monitor. Including misalignment errors and electronic noise, an accurate value of the tune has been derived from statistical treatment repeating this process few hundreds of time.


yoel.giboudot@stfc.ac.uk

 
THPE037 Low Alpha Operation of the Diamond Storage Ring emittance, radiation, storage-ring, electron 4599
 
  • I.P.S. Martin, G. Rehm, J. Rowland, C.A. Thomas
    Diamond, Oxfordshire
  • R. Bartolini, I.P.S. Martin
    JAI, Oxford
 
 

The Diamond storage ring has been operated in low alpha mode providing short-pulse radiation for pump-probe experiments and coherent radiation for THz/IR measurements. Two lattices have been implemented, with both capable of providing a variable alpha in the range ±2x10-5, down to minimum values well below 1x10-6. The second lattice additionally provides a low emittance of 4nm.rad, compared to 35nm.rad for the first lattice. An overview of operation in low alpha mode is given, along with first measurements of coherent emission at long wavelengths under a variety of conditions.

 
THPE039 Optimization of dipole-field profiles for emittance reduction in storage rings dipole, emittance, damping, storage-ring 4605
 
  • C.-x. Wang, Y. Wang
    ANL, Argonne
  • Y.M. Peng
    IHEP Beijing, Beijing
 
 

Nonuniform dipoles with bending field variation have been studied for reducing storage ring emittance in recent years. According to a new minimum emittance theory, the effects of an arbitrary dipole can be characterized by two parameters. To have a better idea of the potentials of nonuniform dipoles, here we numerically explore the values of these two parameters for optimal emittance reduction.

 
THPE042 Single-stage Bunch Compressor for ILC-SB2009 emittance, wiggler, linac, quadrupole 4611
 
  • A. Latina, N. Solyak
    Fermilab, Batavia
 
 

The Project Management Design Team of the International Linear Collider has recently proposed fundamental changes to the published ILC RDR baseline with the goal of presenting a potential alternate design providing a more cost-effective solution. In this framework a new lattice for the Damping Rings has been presented, shortening the exit bunch length from the RDR value of 9 mm down to 6 mm. The shorter bunch length allowed the adoption of a simpler single-stage bunch compressor, instead of the RDR two-stage compressor. The new single-stage compressor has a compression ratio of 20 and still achieves the nominal RDR value of 0.3 mm bunch length at the Interaction Point. The new design has been optimized to generate the required compression while having a small SR emittance growth, and reduced energy spread. The new lattice and its optimization procedure are presented in this paper.

 
THPE047 Lattice Calibration with Turn-by-turn BPM Data quadrupole, simulation, optics, target 4623
 
  • X. Huang, J.J. Sebek
    SLAC, Menlo Park, California
 
 

Turn-by-turn beam position monitor (BPM) data from multiple BPMs are fitted with a tracking code to calibrate magnet strengths in similar manner as the well known LOCO code. Simulation shows that this method can be a quick and efficient way for optics calibration. The method is applicable to both linacs and ring accelerators. We also show experimental measurement of the transfer matrix with turn by turn BPM data.

 
THPE048 Lattice Modeling for SPEAR3 dipole, quadrupole, sextupole, alignment 4626
 
  • X. Huang, J.A. Safranek
    SLAC, Menlo Park, California
 
 

We use measured or simulated magnetic fields for dipoles and quadrupoles to build a lattice model for SPEAR3. In a non-symplectic approach the phase space coordinate mapping on the fields is based on Runge-Kutta integration of the equation of motion. In a symplectic approach we approximate the fields with proper fringe field models. Complication of the use of rectangular gradient dipoles in SPEAR3 is considered. Results of the model is compared to measurements on the real machine.

 
THPE051 Magnet Optical and Beam Matching Issues in a Medium Energy Beam Transport line of SNS Linac simulation, focusing, quadrupole, optics 4632
 
  • J. G. Wang, Y. Zhang
    ORNL, Oak Ridge, Tennessee
 
 

A Medium Energy Beam Transport line (MEBT) is employed in the SNS linac to match the beam from an RFQ to a DTL and to perform other functions. The MEBT lattice consists of fourteen electromagnetic quadrupoles. The quads have very small aspect ratios (steel length over aperture diameter), and they are densely packed in the lattice. Significant fringe fields and magnetic interference cause difficulties in beam matching. We have performed 3D simulations of the magnets, computed their optical properties, and compared their performance with what predicted by simple hard edge models. This paper reports our findings and possible solutions to the problem.

 
THPE053 Linear and Chromatic Optics Measurements at RHIC optics, injection, quadrupole, coupling 4638
 
  • R. Calaga
    BNL, Upton, Long Island, New York
  • M. Aiba
    PSI-LRF, Villigen, PSI
  • R. Tomás, G. Vanbavinckhove
    CERN, Geneva
 
 

Measurements of chromatic beta-beating were carried out for the first time in the RHIC accelerator during Run 2009. The analysis package developed for the LHC was used to extract the off-momentum optics for injection and top energy. Results from the beam experiments and comparison to the optics model are presented.

 
THPE060 A Compact Ring for the ThomX-ray Source emittance, dipole, electron, wakefield 4650
 
  • A. Loulergue
    SOLEIL, Gif-sur-Yvette
  • C. Bruni, J. Haissinski, M. Joré, M. Lacroix, A. Variola
    LAL, Orsay
 
 

One advantage of X-ray sources based on Compton Back Scattering (CBS) processes is that such compact machines can produce an intense flux of monochromatic X-rays. CBS results from collisions between laser pulses and relativistic electron bunches. Aiming at high X-ray flux, one possible configuration combining a low emittance linear accelerator with a compact storage ring and a high gain laser cavity has been adopted by the ThomX project. We present here the main ring lattice characteristics in terms of baseline optics, possible other tunings such as low or negative momentum compaction, and orbit correction schemes. In addition, non-linear beam dynamics aspects including fringe field components as well as higher multipole tolerances are presented.

 
THPE063 Investigation and Optimization of Transverse Non-linear Beam Dynamics in the High-energy Storage Ring HESR dynamic-aperture, resonance, target, quadrupole 4659
 
  • D.M. Welsch, A. Lehrach, B. Lorentz, R. Maier, D. Prasuhn, R. Tölle
    FZJ, Jülich
 
 

The High-Energy Storage Ring (HESR) is part of the upcoming Facility for Antiproton and Ion Research (FAIR). The HESR will provide antiprotons in the momentum range from 1.5 to 15 GeV/c for the internal target experiment PANDA. The demanding requirements of PANDA in terms of beam quality and luminosity together with a limited production rate of antiprotons call for a long beam life time and a minimum of beam loss. Thus, a sufficiently large dynamic aperture of the HESR is crucial. To provide this, a chromaticity correction scheme for the HESR has been developed to reduce tune spread and thus to minimize the emittance growth caused by betatron resonances. The chromaticity correction scheme has been optimized through dynamic aperture calculations. The estimated field errors of the HESR dipole and quadrupole magnets have been included in the non-linear beam dynamics studies. The ion optical settings of the HESR have been improved using dynamic aperture calculations and frequency map analysis technique. In this presentation comprehensive beam simulations are presented and predictions of long-term stability based on short-term particle tracking and orbit diffusion discussed.

 
THPE076 Effect of the Phase One Insertion Devices in the ALBA Storage Ring insertion, insertion-device, dynamic-aperture, multipole 4695
 
  • Z. Martí, G. Benedetti, D. Einfeld, M. Muñoz
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The synchrotron light source ALBA incorporates 6 insertion devices (2 Apple-II type undulators, 2 plannar in-vacuum undulators, 1 normal conducting multipole wiggler and 1 superconduction multipole wiggler) at the start of operation. The effect of the different IDs in the performance of the facility is evaluated, using several methods (kick maps, hard edge models, dynamic multipoles, …), including a comparison of the agreement of the different models and simulation codes. According to the results, and due mainly to the influence of the superconducting wiggler, a new working point has been selected.

 
THPE094 A Search for Integrable Four-dimensional Nonlinear Accelerator Lattices betatron, octupole, focusing, optics 4743
 
  • S. Nagaitsev
    Fermilab, Batavia
  • V.V. Danilov
    ORNL, Oak Ridge, Tennessee
 
 

Integrable nonlinear motion in accelerators has the potential to introduce a large betatron tune spread to suppress instabilities and to mitigate the effects of space charge and magnetic field errors. To create such an accelerator lattice one has to find magnetic and/or electrtic field combinations leading to a stable integrable motion. This paper presents families of lattices with one invariant where bounded motion can be easily created in large volumes of the phase space. In addition, it presents two examples of integrable nonlinear accelerator lattices, realizable with longitudinal-coordinate-dependent magnetic or electric fields with the stable nonlinear motion, which can be solved in terms of separable variables.

 
THPE095 Quantitative Lattice Optimization using Frequency Map Analysis injection, sextupole, emittance, damping 4746
 
  • C. Steier, W. Wan
    LBNL, Berkeley, California
 
 

Frequency Map Analysis has been used successfully to study accelerator lattices for many years, both in simulations and in experiment. We will present a new application to use the quantitative results of frequency maps (namely the diffusion rates) to optimize the nonlinear properties of lattices. The technique is fairly simple but powerful and has already been used to optimize lattices for example for the NLC and ILC damping rings, as well as the ALS lattice upgrade.

 
THPE103 Sorting Chromatic Sectupoles for Second Order Chromaticity Correction in the RHIC sextupole, focusing, power-supply, resonance 4761
 
  • Y. Luo, W. Fischer, G. Robert-Demolaize, S. Tepikian, D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

In this article, based on the contributions of the chromatic sextupole families to the half-integer resonance driving terms, we discuss how to sort the chromatic sextupoles in the arcs of the Relativistic Heavy Ion Collider (RHIC) to easily and effectively correct the second order chromaticities. We propose an online method with 4 knobs or 4 pairs of chromatic sextupole families to correct second order chromaticities. Numerical simulations support this method and shows that it improves the balance of correction strengths among the sextupole families and avoids reversal of sextupole polarities, as well as yielding larger dynamic apertures for the 2009 RHIC 100 GeV polarized proton run.