Keyword: optics
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MOOBS1 Beam Dynamics Issues in the SNS Linac linac, laser, ion, emittance 12
 
  • A.P. Shishlo
    ORNL, Oak Ridge, Tennessee, USA
 
  Funding: This research is supported by UT-Battelle, LLC for the U. S. Department of Energy under contract No. DE-AC05-00OR22725
A review of the Spallation Neutron Source (SNS) linac beam dynamics is presented. It describes transverse and longitudinal beam optics, losses, activation, and comparison between the initial design and the existing accelerator. The SNS linac consists of normal conducting and superconducting parts. The peculiarities in operations with the superconducting part of the SNS linac (SCL), estimations of total losses in SCL, the possible mechanisms of these losses, and the progress in the transverse matching are discussed.
 
slides icon Slides MOOBS1 [1.270 MB]  
 
MOODN5 Chromaticity Correction for a Muon Collider Optics sextupole, quadrupole, collider, luminosity 79
 
  • E. Gianfelice-Wendt, Y. Alexahin, V.V. Kapin
    Fermilab, Batavia, USA
 
  Funding: Work supported by Fermi Research Alliance, LLC under DE-AC02-07CH11359 with the U.S. DOE
Muon Collider (MC) is a promising candidate for the next energy frontier machine. However, in order to obtain peak luminosity in the 1034cm-2s-1 range the collider lattice design must satisfy a number of stringent requirements. In particular the expected large momentum spread of the muon beam and the very small β* call for a careful correction of the chromatic effects. Here we present a particular solution for the interaction region (IR) optics whose distinctive feature is a three-sextupole local chromatic correction scheme. The scheme may be applied to other future machines where chromatic effects are expected to be large.
 
slides icon Slides MOODN5 [0.554 MB]  
 
MOP015 An X-band Gun Test Area at SLAC gun, emittance, quadrupole, cavity 133
 
  • C. Limborg-Deprey, C. Adolphsen, T.S. Chu, M.P. Dunning, C. Hast, R.K. Jobe, E.N. Jongewaard, A.E. Vlieks, D.R. Walz, F. Wang
    SLAC, Menlo Park, California, USA
  • S.G. Anderson, F.V. Hartemann, T.L. Houck, R.A. Marsh
    LLNL, Livermore, California, USA
 
  Funding: Work supported by the U.S. DOE Contract No. DE-AC03-76SF00515
The XTA (X-Band Test Area) is being assembled in the NLCTA tunnel of the SLAC National Laboratory to serve as a test facility for new RF guns. The first gun to be tested will be an upgraded version of the 5.6 cell, 200MV/m peak field X-band designed at SLAC in 2003 for the Compton Scattering experiment run in ASTA. This new version includes some features implemented in 2006 on the LCLS gun such as racetrack couplers, increased mode separation and elliptical irises. These upgrades were discussed in collaboration with LLNL since the same gun will be used as a driver for the LLNL Gamma-ray Source. Our beamline includes an X-band accelerating section which takes the electron beam up to 100 MeV and an electron beam measurement station. Other X-Band guns such as the UCLA Hybrid gun will be characterized at our facility.
 
 
MOP022 The Expected Performance of MICE Step IV emittance, scattering, solenoid, lattice 151
 
  • T. Carlisle, J.H. Cobb
    JAI, Oxford, United Kingdom
 
  Funding: STFC
The international Muon Ionization Cooling Experiment (MICE), under construction at the Rutherford Appleton Laboratory in Oxfordshire (UK), is a test of a prototype cooling channel for a future Neutrino Factory. The experiment aims to achieve, using liquid hydrogen absorbers, a 10% reduction in transverse emittance, measured to an accuracy of 1% by two scintillating fibre trackers within 4 T solenoid fields. Step IV of MICE will begin in 2012, producing the experiment's first cooling measurements. Step IV uses an absorber focus coil module, placed between the two trackers, to house liquid hydrogen or solid absorbers. The performance of Step IV using various absorber materials was simulated. Multiple scattering in high Z absorbers was found to mismatch the beam with the lattice optics, which was largely corrected by re-tuning the MICE lattice accordingly.
 
 
MOP036 Epicyclic Twin-Helix Ionization Cooling Simulations resonance, quadrupole, simulation, betatron 163
 
  • A. Afanasev
    Hampton University, Hampton, Virginia, USA
  • Y.S. Derbenev, V.S. Morozov
    JLAB, Newport News, Virginia, USA
  • V. Ivanov, R.P. Johnson
    Muons, Inc, Batavia, USA
 
  Funding: Supported in part by DOE SBIR grant DE-SC0005589
Parametric-resonance Ionization Cooling (PIC) is proposed as the final 6D cooling stage of a high-luminosity muon collider. For the implementation of PIC, we earlier developed an epicyclic twin-helix channel with correlated behavior of the horizontal and vertical betatron motions and dispersion. We now insert absorber plates with short energy-recovering units located next to them at the appropriate locations in the twin-helix channel. We first demonstrate conventional ionization cooling in such a system with the optics uncorrelated. We then adjust the correlated optics state and induce a parametric resonance to study ionization cooling under the resonant condition.
 
 
MOP052 Matched Optics of Muon RLA and Non-Scaling FFAG ARCS linac, quadrupole, lattice, dynamic-aperture 196
 
  • V.S. Morozov, S.A. Bogacz, Y. Roblin
    JLAB, Newport News, Virginia, USA
  • K.B. Beard
    Muons, Inc, Batavia, USA
  • D. Trbojevic
    BNL, Upton, Long Island, New York, USA
 
  Funding: Supported in part by US DOE STTR Grant DE-FG02-08ER86351
Recirculating Linear Accelerators (RLA) are an efficient way of accelerating short-lived muons to multi-GeV energies required for Neutrino Factories and TeV energies required for Muon Colliders. To reduce the number of required return arcs, we employ a Non-Scaling Fixed-Field Alternating-Gradient (NS-FFAG) arc lattice design. We present a complete linear optics design of a muon RLA with two-pass linear NS-FFAG droplet return arcs. The arcs are composed of symmetric cells with each cell designed using combined function magnets with dipole and quadrupole magnetic field components so that the cell is achromatic and has zero initial and final periodic orbit offsets for both passes’ energies. Matching to the linac is accomplished by adjusting linac quadrupole strengths so that the linac optics on each pass is matched to the arc optics. We adjust the difference of the path lengths and therefore of the times of flight of the two momenta in each arc to ensure proper synchronization with the linac. We investigate the dynamic aperture and momentum acceptance of the arcs.
 
 
MOP072 Design of On-Chip Power Transport and Coupling Components for a Silicon Woodpile Accelerator coupling, laser, electron, simulation 241
 
  • Z. Wu, E.R. Colby, C. McGuinness, C.-K. Ng
    SLAC, Menlo Park, California, USA
 
  Three-dimensional woodpile photonic bandgap (PBG) waveguide enables high-gradient and efficient laser driven acceleration, while various accelerator components, including laser couplers, power transmission lines, woodpile accelerating and focusing waveguides, and energy recycling resonators, can be potentially integrated on a single monolithic structure via lithographic fabrications. This paper will present designs of this on-chip accelerator based on silicon-on-insulator (SOI) waveguide. Laser power is coupled from free-space or fiber into SOI waveguide by grating structures on the silicon surface, split into multiple channels to excite individual accelerator cells, and eventually gets merged into the power recycle pathway. Design and simulation results will be presented regarding various coupling components involved in this network.  
 
MOP088 A High Transformer Ratio Plasma Wakefield Accelerator Scheme for FACET plasma, simulation, wakefield, electron 265
 
  • R.J. England, J.T. Frederico, M.J. Hogan
    SLAC, Menlo Park, California, USA
  • W. An, C. Joshi, W. Lu, W.B. Mori
    UCLA, Los Angeles, California, USA
  • P. Muggli
    USC, Los Angeles, California, USA
 
  Funding: Work supported by the U.S. Department of Energy under contract number DE-AC02-76SF00515
The ideal drive beam current profile for the plasma wakefield accelerator (PWFA) has been predicted by 1D and 2D simulations to be characterized by a triangular ramp that rises linearly from head to tail, followed by a sharp drop. A technique for generating such bunches experimentally was recently demonstrated. We present here an adaptation of this scheme to generate ramped bunches using the 23 GeV electron beam produced in the first two-thirds of the SLAC linac, and discuss plans to implement this scheme for high transformer ratio demonstration experiments at the FACET plasma wakefield accelerator facility.
 
 
MOP090 Optics Tuning Knobs for FACET quadrupole, plasma, wakefield, focusing 268
 
  • Y. Nosochkov, M.J. Hogan, W. Wittmer
    SLAC, Menlo Park, California, USA
 
  Funding: Work supported by the Department of Energy Contract DE-AC02-76SF00515.
FACET is a new facility under construction at the SLAC National Accelerator Laboratory. The FACET beam line is designed to provide 23 GeV tightly focused and compressed electron and positron bunches for beam driven plasma wakefield acceleration research and other experiments. Achieving optimal beam parameters for various experimental conditions requires the optics capability for tuning in a sufficiently wide range. This will be achieved by using optics tuning systems (knobs). Design of such systems for FACET is discussed.
 
 
MOP165 Bringing Accelerator Models to the Control System Studio controls, EPICS, booster, status 403
 
  • N. Malitsky, K. Shroff
    BNL, Upton, Long Island, New York, USA
  • C. Xiaomeng
    Stony Brook University, Stony Brook, USA
 
  This paper is the next logical step in the evolution of the new EPICS-based high-level accelerator application environment. The project presents the connection of its middle layers servers with the new Eclipse-based operational toolkit, Control System Studio. The approach is illustrated by the implementation of the Model Independent Analysis application involving three key servers: Machine, Online Model, and Virtual Accelerator.  
 
MOP179 Numerical Study on Zone Plate Imaging electron, radiation, synchrotron 423
 
  • I.S. Ko
    POSTECH, Pohang, Kyungbuk, Republic of Korea
  • J.Y. Huang, Y.W. Parc
    PAL, Pohang, Kyungbuk, Republic of Korea
 
  Funding: This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Ministry of Education, Science and Technology (MEST) (grant No. R0A-2008-000-20013-0).
The X-ray is focused by two zone plates in 1B2 beamline to image electron beam in PLS. From numerical study, we can determine the optical limit of resolution with the same specifications of Fresnel zone plates in 1B2 beamline. The width of Airy pattern and the outmost width of zone plates are turned out to be not good parameters to determine the resolution of the imaging system with a zone plate. The resolution of the entire imaging system 1B2 beamline will be revealed as 682 nm.
 
 
MOP194 A Laser-Wire Beam-Energy and Beam-Profile Monitor at the BNL Linac electron, laser, linac, ion 456
 
  • R. Connolly, L. DeSanto, C. Degen, R.J. Michnoff, M.G. Minty, D. Raparia
    BNL, Upton, Long Island, New York, USA
 
  Funding: Work performed under Contract #DE-AC02-98CH10886 under the auspices of the US Department of Energy.
In 2009 a beam-energy monitor was installed in the high energy beam transport (HEBT) line at the Brookhaven National Lab linac. This device measures the energies of electrons stripped from the 40mA H beam by background gas. Electrons are stripped by the 1.7x10-7torr residual gas at a rate of ~2.4x10-8/cm. Since beam electrons have the same velocities as beam protons, the beam proton energy is deduced by multiplying the electron energy by mp/me=1836. A 183.6MeV H beam produces 100keV electrons. In 2010 we installed an optics plates containing a laser and optics to add beam-profile measurement capability via photodetachment. Our 100mJ/pulse, Q-switched laser neutralizes 70% of the beam during its 10ns pulse. The chamber in which the laser light passes through the ion beam is upstream of a dipole magnet which deflects the electrons into a biased retarding-grid (V<125kV) Faraday-cup detector. To measure beam profiles, a narrow laser beam is stepped across the ion beam removing electrons from the portion of the H beam intercepted by the laser. The laser also gives us energy measurements on the 0.2mA polarized proton beam.
 
 
MOP199 NSLS-II X-ray Diagnostics Development diagnostics, radiation, electron, wiggler 468
 
  • P. Ilinski
    BNL, Upton, Long Island, New York, USA
 
  NSLS-II storage ring will have less then 1nm*rad emittance. A concept of X-ray diagnostics beamline was developed in order to measure small sizes of radiation sources to deduct beam emittance. Diagnostics will include pinhole cameras and Compound Refractive Lens focusing optics. A novel optical layout was suggested in order to measure sources with large horizontal to vertical aspect ratio.  
 
MOP219 Initial Beam-Profiling Tests with the NML Prototype Station at the Fermilab A0 Photoinjector radiation, emittance, diagnostics, target 510
 
  • A.H. Lumpkin, M.D. Church, R.H. Flora, A.S. Johnson, J. Ruan, J.K. Santucci, V.E. Scarpine, Y.-E. Sun, R.M. Thurman-Keup, M. Wendt
    Fermilab, Batavia, USA
 
  Funding: Operated by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the United States Department of Energy.
Beam-profile diagnostics are being developed for a superconducting (SC) radiofrequency (RF) Test Accelerator that is currently under construction at the New Muon Lab (NML) at Fermilab. The facility’s design goals include the replication of the pulse train proscribed for the International Linear Collider (ILC). An RF photoelectric gun based on the DESY design will generate the beam. In test-beam mode a low-power beam will be characterized with intercepting radiation converter screens: either a 100-micron thick YAG:Ce single crystal scintillator or a 1-micron thin Al optical transition radiation (OTR) foil. This prototype station was constructed by RadiaBeam Technologies under a contract with Fermilab. In both cases the screen surface was normal to the beam direction followed by a downstream 45-degree mirror that directed the radiation into the optical system. The optical system has better than 20 (10) micron rms spatial resolution when covering a vertical field of view of 18(5) mm. These initial tests were performed at the A0 Photoinjector at a beam energy of ~15 MeV and with micropulse charges from 25 to 500 pC for beam sizes of 45 to 250 microns. Example results will be presented.

 
 
MOP221 An Application for Tunes and Coupling Evaluation From Turn-by-Turn Data at the Fermilab Booster coupling, booster, resonance, controls 516
 
  • W.L. Marsh, Y. Alexahin, E. Gianfelice-Wendt
    Fermilab, Batavia, USA
 
  Funding: Work supported by Fermi Research Alliance, LLC under DE-AC02-07CH11359 with the U.S. DOE.
A console application using the phasing of Turn-by-Turn signals from the different BPMs has been tested at the Fermilab Booster. This techinique allows the on-line detection of the beam tunes during the fast Booster ramp in conditions where other algorithms were unsuccessful. The application has been recently expanded to include the computation of the linear coupling coefficients. Algorithm and measurement results are presented.
 
 
MOP239 Commercially Available Transverse Profile Monitors, the IBIS target, vacuum, diagnostics, impedance 562
 
  • M. Ruelas, R.B. Agustsson, I. Bacchus, A.Y. Murokh, R. Tikhoplav
    RadiaBeam, Santa Monica, USA
 
  With ever decreasing budgets, shorter delivery schedules and increased performance requirements for pending and future facilities, the need for cost effective yet high quality profile monitors is paramount to future advancement in the accelerator field. While individual facilities are capable of designing and fabricating these often custom devices, this is not always the most efficient or economical route. In response to the lack of commercially available profile monitors, RadiaBeam Technologies has been developing its line of Integrated Beam Imaging System (IBIS) over the past several years. Here, we report on these commercially available profile monitors.  
 
MOP304 Development of an X-Ray Beam Size Monitor with Single Pass Measurement Capability for CesrTA electron, positron, photon, controls 687
 
  • N.T. Rider, J.P. Alexander, M.G. Billing, J. Dobbins, R.E. Meller, M.A. Palmer, D.P. Peterson, C.R. Strohman
    CLASSE, Ithaca, New York, USA
  • J.W. Flanagan
    KEK, Ibaraki, Japan
 
  The CESR Test Accelerator (CesrTA) program targets the study of beam physics issues relevant to linear collider damping rings. This endeavor requires new instrumentation to study the beam dynamics along trains of ultra low emittance bunches. A key element of the program has been the development of an x-ray beam size monitor capable of collecting single pass measurements of individual bunches in a train over thousands of turns. This instrument utilizes custom, high bandwidth amplifiers and digitization hardware to collect signals from a linear InGaAs diode array. The digitizer is synchronized with the CESR timing system and is capable of recording beam size measurements for bunches spaced by as little as 4ns. The x-ray source is a bending magnet with Ec=0.6 keV during 2 GeV CesrTA operations. For these conditions the amplifier dynamic range was optimized to allow measurements with 3x109 to 1011 particles per bunch. Initial testing is complete. Data analysis and examples of key measurements which illustrate the instrument's performance are presented. This device offers unique measurement capabilities applicable to future high energy physics accelerators and light sources.  
 
TUP235 Strategy for Neutralizing the Impact of Insertion Devices on the MAX IV 3 GeV Ring storage-ring, multipole, lattice, vacuum 1262
 
  • E.J. Wallén, S.C. Leemann
    MAX-lab, Lund, Sweden
 
  In order to prepare for the potentially negative influence on the beam lifetime, injection efficiency and beam size from the insertion devices (IDs) on the stored beam of the MAX IV 3 GeV storage ring strategy for neutralizing the foreseen effects of the IDs has been developed. In short the strategy involves a local correction of the betatron phase advance by adjusting the strength of the quadrupoles adjacent to the ID. There will also be a global tune correction in order to avoid drift in the working point of the storage ring during operation. Air coils with empirical feed forward tables for the excitation current in the coils will compensate for field integral errors. The lattice of the MAX IV 3 GeV storage ring appears to be robust and it tolerates the dynamic multipoles created by the expected initial set of IDs provided that the local correction of the betatron phase advance has been carried out.  
 
WEOAN1 Accelerator Timing Systems Overview controls, laser, kicker, FEL 1376
 
  • J. Serrano, P. Alvarez, M.M. Lipinski, T. Włostowski
    CERN, Geneva, Switzerland
 
  Timing systems are crucial ingredients for the successful operation of any particle accelerator complex. They are used not only to synchronize different processes but also to time-stamp and ensure overall coherency of acquired data. We describe fundamental time and frequency figures of merit and methods to measure them, and continue with a description of current synchronization solutions for different applications, precisions and geographical coverage, and some examples. Finally, we describe new trends in timing technology and applications.  
slides icon Slides WEOAN1 [1.122 MB]  
 
WEP005 Modeling the Low-Alpha-Mode at ANKA with the Accelerator Toolbox quadrupole, synchrotron, sextupole, dipole 1510
 
  • M. Klein, N. Hiller, A. Hofmann, E. Huttel, V. Judin, B. Kehrer, S. Marsching, A.-S. Müller
    KIT, Karlsruhe, Germany
  • K.G. Sonnad
    CLASSE, Ithaca, New York, USA
 
  The ANKA storage ring is operated frequently with low momentum compaction lattices to produce short bunches for the generation of coherent synchrotron radiation in the THz range. The bunch length can be varied in steps from one centimeter down to the sub millimeter level. These low alpha optics are modeled by using the Matlab based tools, Accelerator Toolbox (AT) and LOCO. The results are compared with measurements such as orbit response matrices, dispersion and chromaticity. This paper provides results of a study on the feasibilities as well as limitations of the measurements and calculations.  
 
WEP033 Using an Emittance Exchanger as a Bunch Compressor emittance, cavity, coupling, simulation 1555
 
  • B.E. Carlsten, K. Bishofberger, L.D. Duffy, Q.R. Marksteiner, S.J. Russell, N.A. Yampolsky
    LANL, Los Alamos, New Mexico, USA
 
  Funding: This work is supported by the U.S. Department of Energy through the LANL/LDRD program.
An Emittance EXchanger (EEX), like a chicane, can be used for bunch compression. However, it offers a unique characteristic: the R56 term in an EEX vanishes, which decouples the final longitudinal position from the particles’ energies, thereby suppressing the microbunch instability. Also, it can provide simultaneous compression in both the longitudinal and one transverse dimensions, where, for example, the final longitudinal size is smaller than the initial horizontal size and the final horizontal size is smaller than the initial longitudinal size. In this scheme, there is no dependence on an energy slew needed for compressing the beam, simplifying the rf requirements. A bunch-compression scheme using two EEXs is presented, including CSR calculations.
 
 
WEP035 Intense Sheet Electron Beam Transport in a Periodically Cusped Magnetic Field focusing, electron, simulation, gun 1558
 
  • P.B. Larsen, B. Levush, J.A. Pasour
    NRL, Washington, DC, USA
  • T.M. Antonsen
    UMD, College Park, Maryland, USA
  • A.T. Burke, J.J. Petillo
    SAIC, Billerica, Massachusetts, USA
  • K.T. Nguyen
    Beam-Wave Research, Inc., Union City, USA
 
  Funding: Acknowledgements: We gratefully acknowledge funding by the Office of Naval Research.
We explore periodically cusped magnetic (PCM) fields in the regime of a Ka-Band coupled-cavity travelling wave tube (beam current = 3.5A, voltage = 19.5kV, 10:1 beam aspect ratio). We use finite-element beam optics code MICHELLE to simulate the 3-dimensional beam optics for the beam transport within a PCM field. Realistic 3-dimensional magnetic fields have been considered to determine the practicality of these designs. We present the methodology used to focus and transport a thermal beam from a shielded-cathode, high aspect-ratio electron gun.
 
 
WEP044 Emittance and Phase Space Exchange cavity, emittance, quadrupole, lattice 1576
 
  • D. Xiang, A. Chao
    SLAC, Menlo Park, California, USA
 
  Funding: This work was supported by the US DOE under Contract No. DE-AC02-76SF00515.
Alternative chicane-type beamlines are proposed for exact emittance exchange between horizontal phase space (x,x') and longitudinal phase space (z, delta). Methods to achieve exact phase space exchanges, i.e. mapping x to z, x' to delta, z to x and delta to x' are suggested. Some applications of the phase space exchanger and the feasibility of an emittance exchange experiment with the proposed beamline at SLAC are discussed.
 
 
WEP048 Comparison of RF Cavity Transport Models for BBU Simulations linac, cavity, focusing, simulation 1582
 
  • I. Shin
    University of Connecticut, Storrs, Connecticut, USA
  • S. Ahmed, T. Satogata, B.C. Yunn
    JLAB, Newport News, Virginia, USA
 
  The transverse focusing effect in RF cavities plays a considerable role in beam dynamics for low-energy beamline sections and can contribute to beam breakup (BBU) instability. The purpose of this analysis is to examine RF cavity models in simulation codes which will be used for BBU experiments at Jefferson Lab and improve BBU simulation results. We review two RF cavity models in the simulation codes elegant and TDBBU (a BBU simulation code developed at Jefferson Lab). elegant can include the Rosenzweig-Serafini (R-S) model for the RF focusing effect. Whereas TDBBU uses a model from the code TRANSPORT which considers the adiabatic damping effect, but not the RF focusing effect. Quantitative comparisons are discussed for the CEBAF beamline. We also compare the R-S model with the results from numerical simulations for a CEBAF-type 5-cell superconducting cavity to validate the use of the R-S model as an improved low-energy RF cavity transport model in TDBBU. We have implemented the R-S model in TDBBU. It will cause BBU simulation results to be better matched with analytic calculations and experimental results.  
 
WEP070 Ring for Test of Nonlinear Integrable Optics betatron, lattice, quadrupole, multipole 1606
 
  • A. Valishev, V.S. Kashikhin, S. Nagaitsev
    Fermilab, Batavia, USA
  • V.V. Danilov
    ORNL, Oak Ridge, Tennessee, USA
 
  Funding: Work supported by UT-Battelle, LLC and by FRA, LLC for the U. S. DOE under contracts No. DE-AC05-00OR22725 and DE-AC02-07CH11359 respectively.
Nonlinear optics is a promising idea potentially opening the path towards achieving super high beam intensities in circular accelerators. Creation of a tune spread reaching 50% of the betatron tune would provide strong Landau damping and make the beam immune to instabilities. Recent theoretical work* have identified a possible way to implement stable nonlinear optics by incorporating nonlinear focusing elements into a specially designed machine lattice. In this report we propose the design of a test accelerator for a proof-of-principle experiment. We discuss possible studies at the machine, requirements on the optics stability and sensitivity to imperfections.
* V. Danilov and S. Nagaitsev, Phys. Rev. ST Accel. Beams 13, 084002 (2010)
 
 
WEP150 GPU Computing for Particle Tracking dynamic-aperture, simulation, lattice, storage-ring 1764
 
  • H. Nishimura, S. James, K. Muriki, Y. Qin, K. Song, C. Sun
    LBNL, Berkeley, California, USA
 
  Funding: Work supported by the U.S. Department of Energy under Contract No. DE-AC02-05CH11231
This is a feasibility study of using a modern Graphics Processing Unit (GPU) to parallelize the accelerator particle tracking code. To demonstrate the massive parallelization features provided by GPU computing, a simplified TracyGPU program is developed for dynamic aperture calculation. Performances, issues, and challenges from introducing GPU are also discussed.
 
 
WEP293 Design and Fabrication of the Lithium Beam Ion Injector for NDCX-II ion, ion-source, vacuum, solenoid 2032
 
  • J.H. Takakuwa, J.-Y. Jung, J.T. Kehl, J.W. Kwan, M. Leitner, P.A. Seidl, W.L. Waldron
    LBNL, Berkeley, California, USA
  • A. Friedman, D.P. Grote, W. M. Sharp
    LLNL, Livermore, California, USA
 
  Funding: This work is performed under the auspices of the U.S. Department of Energy by LBNL under contract DE-AC02-05CH11231.
A 130 keV injector is developed for the NDCX-II facility. It consists of a 10.9 cm diameter lithium doped alumina-silicate ion source heated to ~1300 °C and 3 electrodes. Other components include a segmented Rogowski coil for current and beam position monitoring, a gate valve, pumping ports, a focusing solenoid, a steering coil and space for inspection and maintenance access. Significant design challenges including managing the 3-4 kW of power dissipation from the source heater, temperature uniformity across the emitter surface, quick access for frequent ion source replacement, mechanical alignment with tight tolerance, and structural stabilization of the cantilevered 27” OD graded HV ceramic column. The injector fabrication is scheduled to complete by May 2011, and assembly and installation is scheduled to complete by the beginning of July.
 
 
WEP295 Status of Laser Stripping at the SNS laser, linac, quadrupole, injection 2035
 
  • T.V. Gorlov, A.V. Aleksandrov, V.V. Danilov
    ORNL, Oak Ridge, Tennessee, USA
  • Y. Liu
    ORNL RAD, Oak Ridge, Tennessee, USA
 
  Funding: This work was supported by SNS through UT-Battelle, LLC, under Contract No. DE-AC05-00OR22725 for the U.S. Department of Energy.
This paper presents an overview of experimental and theoretical studies on laser stripping that have been conducted up to the present time in the SNS project. The goal of this work is to develop techniques to achieve the experimental preconditions necessary for the successful realization of a future intermediate experiment on laser stripping. The experimental work consists of the tuning and measurement of H־ beam parameters in readiness for the intermediate experiment, and also takes into account the features and possibilities of the SNS accelerator.
 
 
THP016 Design of an Achromatic and Uncoupled Medical Gantry for Radiation Therapy quadrupole, dipole, radiation, controls 2163
 
  • N. Tsoupas, D. Kayran, V. Litvinenko, W.W. MacKay
    BNL, Upton, Long Island, New York, USA
 
  Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.
We are presenting the layout and the optics of a beam line to be used as a medical gantry in radiation therapy. The optical properties of the gantry’s beam line are such as to make the beam line achromatic and uncoupled. These two properties make the beam spot size, which is delivered and focused by the gantry, on the tumor of the patient, independent of the angular orientation of the gantry. In this paper we present the layout of the magnetic elements of the gantry, and also present the theoretical basis for the optics design of such a gantry.
* N. Tsoupas et. al. “Uncoupled achromatic tilted S-bend” Presented at the 11th Biennial European Particle Accelerator Conference, Genoa, Italy, June 23-27,2008
 
 
THP125 Multi-objective Optimization of a Lattice for Potential Upgrade of the Advanced Photon Source* lattice, sextupole, dynamic-aperture, quadrupole 2354
 
  • V. Sajaev, M. Borland, L. Emery, A. Xiao
    ANL, Argonne, USA
 
  Funding: *Work supported by the U. S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.
The Advanced Photon Source (APS) is a 7-GeV storage ring light source that has been in operation for over a decade. In the near future, the ring may be upgraded, including changes to the lattice such as provision of several long straight sections (LSSs). Use of deflecting cavities for generation of short x-ray pulses is also considered. Because APS beamlines are nearly fully built out, we have limited freedom to place LSSs in a symmetric fashion. Arbitrarily placed LSSs will drastically reduce the symmetry of the optics and would typically be considered unworkable. We apply a recently developed multi-objective direct optimization technique that relies on particle tracking to compute the dynamic aperture and Touschek lifetime. We show that this technique is able to tune sextupole strengths and select the working point in such a way as to recover the dynamic and momentum acceptances. We also show the results of experimental tests of lattices developed using these techniques.
 
 
FROAN2 DIANA, a Next Generation Deep Underground Accelerator Facility ion, target, background, solenoid 2552
 
  • D. Leitner
    NSCL, East Lansing, Michigan, USA
  • M. Couder, M. Wiescher
    Notre Dame University, Notre Dame, Iowa, USA
  • A. Hodgkinson, A. Lemut, J.S. Saba
    LBNL, Berkeley, California, USA
  • M. Leitner
    FRIB, East Lansing, Michigan, USA
 
  Funding: This work was supported by the National Science Foundation NSF-09-500 grant (DUSEL S4), Proposal ID 091728
DIANA (Dakota Ion Accelerators for Nuclear Astrophysics) is a next generation nuclear astrophysics accelerator facility proposed to be built as part of the US DUSEL (Deep Underground Science and Engineering Laboratory) project. The scientific goals of DIANA are focused on experiments related to nucleosynthesis processes. Reaction cross-sections at stellar temperature are extremely low, which makes these experiments challenging. Small signal rates are overwhelmed by large background rates associated with cosmic ray-induced reactions, background from natural radioactivity in the laboratory environment, and the beam-induced background on target impurities. By placing the DIANA facility deep underground (1.4 km) the cosmic ray induced background can be eliminated. In addition, the DIANA accelerator is being designed to achieve large laboratory reaction rates by delivering high ion beam currents (up to 100 mA) to a high density super-sonic jet-gas target (up to 1018 atoms/cm2). Two accelerators are coupled to enable measurements over a wide energy range from 30 keV to 3 MeVin a consistent manner. The accelerators design and its technical challenges are presented.
 
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