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beam-transport

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MOXKI03 Status of the SNS - Machine and Science linac, target, beam-losses, injection 7
 
  • S. Henderson
  Funding: ORNL/SNS is managed by UT-Battelle, LLC, for the U. S. Department of Energy under contract DE-AC05-00OR22725.

The Spallation Neutron Source (SNS) will be the world's leading pulsed neutron source, with design beam power capability of 1.4 MW. The SNS Construction Project was completed in June 2006. The accelerator complex was successfully commissioned during the construction phase of the project in seven discrete commissioning runs. The facility is now in the first of a three year performance ramp-up phase, in which the beam power, reliability and operating time will be increased to the baseline design values of 1.4 MW, 90% and 5000 hours respectively. Meanwhile, neutron scattering instruments are being constructed and commissioned in preparation for full user operations in 2009. The progress toward bringing the SNS to its full capabilities will be presented.

 
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MOZBKI03 The JLab 12 GeV Energy Upgrade of CEBAF for QCD and Hadronic Physics linac, controls, electron, emittance 58
 
  • L. S. Cardman
  • L. Harwood
    Jefferson Lab, Newport News, Virginia
  Funding: Authored by Jefferson Science Associates, LLC under U. S. DOE Contract No. DE-AC05-06OR23177

CEBAF is a 5-pass, recirculating cw electron linac operating at ~6 GeV. The 12-GeV Upgrade is a $300M project anticipated to receive Critical Decision 2 approval in late summer of 2007 and begin construction activities in 2008; funding for the project is provided by the DOE Office of Nuclear Physics which will double the beam energy. The new energy reach will permit significant extensions in research into non-perturbative aspects of QCD. Areas of interest are Generalized Parton Distributions (GPDs), measurements at high-xBjorken, and the use of hybrid mesons to explore the nature of quark confinement. The upgrade includes: doubling the accelerating voltages of the linacs by adding 10 new high-performance cryomodules plus the requisite expansion of the 2K cryogenics plant and rf power systems, upgrading the beam transport system from 6 GeV to 12 GeV capability through extensive re-use of existing hardware, adding one recirculation arc, adding a new experimental area and the beamline to it, building new experimental equipment for the GPD, high-xBjorken, and hybrid mesons programs. The presentation will touch on the science and give some details of the accelerator plans.

 
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MOPAN031 Design Study of a Very Large Aperture Eddy Current Septum for J-PARC septum, injection, linac, extraction 224
 
  • K. Fan
  • H. Kobayashi, H. Matsumoto, Y. Sakamoto
    KEK, Ibaraki
  An eddy current septum is selected as a backup of injection septum. Due to the high beam intensity and low beam energy, the injection beam size is very large. To accommodate the large size beam, large aperture septum is required. Large end field and large eddy current loss result in degradation of gap field. The paper discusses the eddy current loss effects on field distribution and introduces some correction methods.  
 
TUZBAB02 The Extreme Value Theory to Estimate Beam Losses in High Power Linacs linac, beam-losses, quadrupole, simulation 815
 
  • R. Duperrier
  • D. Uriot
    CEA, Gif-sur-Yvette
  The influence of random perturbations of high intensity accelerator elements on the beam losses is considered. This influence is analyzed with the help of the Extreme Value Theory (EVT) to allow loss estimates for a very low fraction of the beam. Many fields of modern science and engineering have to deal with events which are rare but have significant consequences. EVT is considered to provide the basis for the statistical modeling of such extremes events (extreme variations of financial market for insurance companies or extreme wind speed for electric companies). To illustrate the application of this theory to beam losses estimates, the SPIRAL2 driver is used. This 5 mA deuteron accelerator is simulated from the output of the source to the target with high resolution PIC modelisations (up to 1.3 million macro-particles) using realistic external fields.  
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TUXC01 Status of DARHT 2nd Axis Accelerator at the Los Alamos National Laboratory target, electron, kicker, induction 831
 
  • R. D. Scarpetti
  • J. Barraza, C. Ekdahl, E. Jacquez, S. Nath, K. Nielsen, G. J. Seitz
    LANL, Los Alamos, New Mexico
  • F. M. Bieniosek, B. G. Logan
    LBNL, Berkeley, California
  • G. J. Caporaso, Y.-J. Chen
    LLNL, Livermore, California
  This presentation will provide a status report on the 2kA, 17MeV, 2-microsecond Dual-Axis Radiographic Hydrotest electron beam accelerator at Los Alamos National Laboratory, and will cover results from the cell refurbishment effort, commissioning experiments on beam transport and stability through the accelerator, and experiments exercising the beam chopper.  
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TUPMN119 Energy Recovery Transport Design for Peking University FEL wiggler, electron, recirculation, laser 1191
 
  • G. M. Wang
  • Y.-C. Chao
    Jefferson Lab, Newport News, Virginia
  • J.-E. Chen, C. Liu, Z. C. Liu, X. Y. Lu, K. Zhao, J. Zhuang
    PKU/IHIP, Beijing
  Funding: supported by National 973 Projects and the U. S. Department of Energy Contract No. DE-AC05-06OR23177

A free-electron laser based on a superconducting linac is under construction in Peking University. To increase FEL output power, energy recovery is chosen as one of the most potential and popular ways. The design of a beam transport system for energy recovery is presented, which is suitable for the Peking University construction area. Especially, a chicane structure is chosen to change path length at ±20 degree and M56 in the arc is adjusted for fully bunch compression.

 
 
TUPMS058 The LCLS Injector Drive Laser laser, cathode, gun, controls 1317
 
  • W. E. White
  • J. Castro, P. Emma, A. Gilevich, C. Limborg-Deprey, H. Loos, A. Miahnahri
    SLAC, Menlo Park, California
  Requirements for the LCLS injector drive laser present significant challenges to the design of the system. While progress has been demonstrated in spatial shape, temporal shape, UV generation and rep-rate, a laser that meets all of the LCLS specifications simultaneously has yet to be demonstrated. These challenges are compounded by the stability and reliability requirements. The drive laser and transport system has been installed and tested. We will report on the current operational state of the laser and plans for future improvements.  
 
TUPAN002 Large Displacement and Divergence Analytic Transfer Maps Through Quadrupoles quadrupole, focusing, lattice, proton 1389
 
  • S. R. Koscielniak
  Funding: TRIUMF receives federal funding via a contribution agreement through the National Research Council of Canada.

Linear-field non-scaling FFAGs are proposed for multi-GeV muon acceleration and order hundred MeV/u proton or carbon medical applications. The periodic lattices, which have large momentum acceptance (factor >3), employ cells comprised of combined function magnets. In one implementation, rectangular-shaped quadrupoles are used, with the dipole component generated by off-setting the magnet centre. This feature, coupled with the large radial aperture, gives rise to orbits with large displacement and/or divergence from the quadrupole centre. The angles may be so large that there is a partial interchange of longitudinal and radial momenta. We examine two methods to devise maps (through the body field) that are third order in radial coordinate and higher order in momentum. The WKBJ approximation is concluded to be no better than the usual linear transfer matrix. A Green's function approach is carried through to non-linear mappings for the dynamical variables, which are coupled. The first partial derivative of this map (relates to tune variation) produces a linear transfer matrix which must have unity determinant. For the FFAG application, the map is comparable with numerical integration.

 
 
TUPAN043 RF Amplitude and Phase Tuning of J-PARC DTL linac, monitoring, injection, controls 1481
 
  • M. Ikegami
  • H. Asano, T. Kobayashi
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  • K. Hasegawa, T. Ito, T. Morishita, S. Sato, A. Ueno
    JAEA/LINAC, Ibaraki-ken
  • Z. Igarashi, H. Tanaka
    KEK, Ibaraki
  • H. Sako
    JAEA, Ibaraki-ken
  The beam commissioning of J-PARC linac has been started in November 2006. In the beam commissioning, the tuning of the RF phase and amplitude for its DTL (Drift Tube Linac) has been performed with a phase-scan method. Detailed results of the RF tuning are presented with a brief discription of the tuning procedure.  
 
TUPAN059 The Precise Survey and the Alignment Results of the J-PARC Linac linac, survey, alignment, laser 1520
 
  • T. Morishita
  • H. Asano, M. Ikegami
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  • K. Hasegawa
    JAEA, Ibaraki-ken
  • A. Ueno
    JAEA/LINAC, Ibaraki-ken
  J-PARC linear accelerator components have been installed and the beam commissioning has been started in Nov. 2006. A total length is more than 400 m including the beam transport line to the 3GeV RCS(Rapid Cycling Synchrotron). Precise alignment of the accelerator components is essential for high quality beam acceleration. After the completion of the linac building, floor elevation was surveyed periodically for more than one year to adjust the beam height from the ion source to the RCS. Before the beam commissioning, a metrological survey has been done. The reference points on the tunnel wall were set up to form a survey network to reduce the survey error less than 1mm in the entire linac. Based on the survey results, the linac components were re-aligned finely to satisfy the requirement. In this paper, the results of the floor elevation and the final alignment are described.  
 
TUPAN115 Comparative Study of Beam Dynamics in LINAC4 using CERN and RAL MEBT (Medium Energy Beam Transport) Lines linac, emittance, quadrupole, simulation 1646
 
  • D. C. Plostinar
  • E. Zh. Sargsyan
    CERN, Geneva
  Funding: We acknowledge the support of the European Community-Research Infrastructure Activity under the FP6 "Structuring the European Research Area" program (CARE, Contract No. RII3-CT-2003-506395).

CERN and RAL are working in parallel to develop Front Ends for future particle accelerators. At CERN the Front End will be part of LINAC4, a potential replacement for the Linac2 accelerator, whilst at RAL the Front End is intended to demonstrate that a high current, high quality chopped beam is achievable and that the design could be used as part of a Proton Driver for a future Neutrino Factory. The two Front End designs have many similarities and basically consist of four main components: an H- ion source, a Low Energy Beam Transport (LEBT) matching into a Radio-Frequency Quadrupole (RFQ) and a Medium Energy Beam Transport (MEBT) line with a fast beam chopper. The beam choppers are different in the two designs and it is important to compare the effectiveness of the two methods of operation. This paper describes a simulation study of high intensity beam dynamics and beam transport when the RAL and CERN MEBT designs are each fed into the same CERN structure for LINAC4.

 
 
TUPAS046 Uniform Beam Intensity Redistribution in the LENS Nonlinear Transport Line octupole, target, proton, simulation 1748
 
  • A. Bogdanov
  • V. Anferov, M. Ball, D. V. Baxter, V. P. Derenchuk, A. V. Klyachko, T. Rinckel, K. A. Solberg
    IUCF, Bloomington, Indiana
  Funding: The LENS project is supported by the NSF (grants DMR-0220560, DMR-0242300), the 21st Century Science and Technology fund of Indiana, Indiana University, and the Department of Defense

The Low Energy Neutron Source (LENS) at Indiana University is producing neutrons by using a 7 MeV proton beam incident on a Beryllium target. The Proton Delivery System is currently being upgraded. A new DTL section will be added to increase proton beam energy from 7 to 13 MeV. A 3 MeV RFQ and 13 MeV DTL will be powered by 1 MW klystrons. The goal of this upgrade is a 13 MeV, 20 mA proton beam with duty factor more than 1%. At this power level it becomes increasingly important to make a proton beam that is uniformly distributed to prevent excessive thermal stress at the surface of the Be target. To achieve this goal two octupole magnets are being implemented in the LENS beam transport line. In this paper we discuss the experimental results of the beam intensity redistribution as well as some features inherent in tuning of the nonlinear beamline and our operational experience.

 
 
TUPAS057 Injector Particle Simulation and Beam Transport in a Compact Linear Proton Accelerator proton, electron, simulation, extraction 1781
 
  • D. T. Blackfield
  • Y.-J. Chen, J. R. Harris, S. D. Nelson, A. Paul, B. R. Poole
    LLNL, Livermore, California
  Funding: This work was performed under the auspices of the U. S. Department of Energy by University of California, Lawrence Livermore National Laboratory under Contract W-7405-Eng-48.

A compact Dielectric Wall Accelerator (DWA), with field gradient up to 100 MV/m, is being developed to accelerate proton bunches for use in cancer therapy treatment. The injector first generates a few nanosecond long and 40 pQ proton bunch, which is then compressed in the compression section at the end of the injector. Finally the bunch is accelerated in the high-gradient DWA accelerator to energy up to 70 - 250 MeV. The Particle-In-Cell (PIC) code LSP is used to model several aspects of this design. First, we use LSP to determine the needed voltage waveform in the A-K gap that will produce a proton bunch with the requisite charge. We then model pulse compression and shaping in the section between the A-K gap and the DWA. We finally use LSP to model the beam transport through the DWA.

 
 
TUPAS073 New Design of the SNS MEBT Chopper Deflector linac, power-supply, extraction, target 1817
 
  • A. V. Aleksandrov
  • C. Deibele
    ORNL, Oak Ridge, Tennessee
  Funding: SNS is managed by UT-Battelle, LLC, under contract DE-AC05-00OR22725 for the U. S. Department of Energy.

The chopper system for the Spallation Neutron Source (SNS) provides a gap in the beam for clean extraction from the accumulator ring. It consists of a pre-chopper in the low energy beam transport and a faster chopper in the medium energy beam transport (MEBT). The original "meander line" design of the MEBT chopper deflector was successfully tested with low power beam during the SNS linac commissioning but turned out to be unsuitable for high power beam operation due to poor cooling of the copper strip line through the dielectric substrate. We developed a new deflecting structure, with higher deflection efficiency and with rise and fall time easily customizable to match the available high voltage pulse generator. In this paper we describe design, implementation and beam tests results of the new MEBT chopper deflector.

 
 
WEPMS014 Vacuum Insulator Studies for the Dielectric Wall Accelerator vacuum, electron 2358
 
  • J. R. Harris
  • D. T. Blackfield, G. J. Caporaso, Y.-J. Chen, M. Sanders
    LLNL, Livermore, California
  • M. L. Krogh
    University of Missouri - Rolla, Rolla, Missouri
  Funding: This work was performed under the auspices of the U. S. Department of Energy by the University of California, Lawrence Livermore National Laboratory under Contract No. W-7405-Eng-48.

As part of our ongoing development of the Dielectric Wall Accelerator, we are studying the performance of multilayer high-gradient insulators. These vacuum insulating structures are composed of thin, alternating layers of metal and dielectric, and have been shown to withstand higher gradients than conventional vacuum insulator materials. This paper describes these structures and presents some of our recent results.

 
 
THPMN012 A 0.5 to 50 MeV Electron Linear Accelerator System electron, dipole, quadrupole, bunching 2731
 
  • C. Piel
  • K. Dunkel, C. Schulz
    ACCEL, Bergisch Gladbach
  Since 1998 ACCEL delivers turn key accelerator for scientific applications. After three injector systems for synchrotron light sources have been successfully commissioned, ACCEL is currently producing a 5 to 50 MeV system for the German Metrological Institute in Braunschweig. Beside excellent beam energy qualities the accelerator has to operate in a wide energy range, delivering 1 to 100 W average beam power to the target. The paper will give a description of the system layout and related technical parameters. The status of the project and results of the factory acceptance test of some of the major components will be presented as well.  
 
THPAN003 Image Effects on the Transport of Intense Beams focusing, simulation, multipole, vacuum 3223
 
  • R. Pakter
  • Y. Levin, F. B. Rizzato
    IF-UFRGS, Porto Alegre
  Funding: CNPq and FAPERGS, Brazil, and U. S. AFOSR Grant No. FA9550-06-1-0345.

We start by analyzing the image effects of a cylindrical conducting pipe on a continuous beam with elliptical symmetry. In particular, we derive an exact expression for the self-field potential of the beam inside the pipe without using any sort of multipole expansion. By means of a variational method, the potential for beams with varying density profiles along an elliptical shape is used to search for equilibrium solutions for intense beams. For that, we assume a uniform focusing in the smooth-focusing approximation. A curious result is that the product of the rms sizes along the ellipsis semi-axis stays constant as the pipe radius is varied. Finally, we prove that despite the nonlinear forces imposed by the image charges of an arbitrary shape conducting pipe, intense beams in uniform focusing fields preserve a uniform density in the equilibrium.

 
 
THPAN005 Short Quadrupole Parametrization quadrupole, focusing, kaon, simulation 3229
 
  • A. Baartman
  • D. Kaltchev
    TRIUMF, Vancouver
  Funding: National Research Council (Canada)

The Enge function can be used to parametrize any element with well-defined edges. If an element is too short, however, there is no unambiguous definition of the effective edge. We first demonstrate that very little fringe field detail is needed to obtain accurate maps even up to fifth order. Then we go on to show a simple fitting algorithm that works well for short as well as long quadrupoles. The results are true whether the quads are magnetic or electrostatic.

 
 
THPAN013 Computer-assisted Electron Beam Characterization at AIRIX Facility diagnostics, electron, cathode, extraction 3250
 
  • O. Mouton
  • M. Caron, F. Cartier, D. Collignon, G. Grandpierre, D. Guilhem, L. Hourdin, M. Mouillet, C. Noel, D. Paradis, O. Pierret
    CEA, Pontfaverger-Moronvilliers
  AIRIX is a high current accelerator designed for flash X-ray radiography. The electron beam produced into a vacuum diode (2 kA, 3.5 to 3.8 MV, 60 ns) is extracted from a velvet cold cathode. For a complete beam characterisation at the diode output the following set of data is required: the primary beam current intensity, the primary beam energy, the 2D mean beam divergence, the 2D RMS beam size as well as the 2D transverse beam emittance. Part of these parameters is experimentally given by electrical sensors located into the beam line (I), by time resolved energy spread measurements (E) as well as by a classical beam imaging set-up (XRMS, YRMS). Unfortunately, XRMS and YRMS are measured downstream the diode output. Therefore, in order to get the relevant beam parameters at the right location (diode output) numerical data treatments are required. The TRAJENV beam transport code, coupled with the MINUIT minimization library, computes the unknown beam parameters at the diode output. In this paper, we propose to describe both experimental and theoretical approaches leading to the full beam characterization at the diode output.  
 
THPAN043 Comparison of Trajectory Between Modeling and Experiment for J-PARC Linac linac, quadrupole, simulation, betatron 3324
 
  • T. Ohkawa
  • H. Ao, A. Ueno
    JAEA/LINAC, Ibaraki-ken
  • K. Hasegawa
    JAEA, Ibaraki-ken
  • M. Ikegami
    KEK, Ibaraki
  • H. Sako
    JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken
  In the beam commissioning of J-PARC (Japan Proton Accelerator Research Complex) linac, three simulations codes are used to model the accelerator. We have compared with the experimental results obtained in the beam commissioning to date, where a basic agreement has been confirmed between the modeling and the actual beam behavior.  
 
THPAN049 Particle Dynamics at Stagnation Point during Longitudinal Bunch Compression of High Current Beams emittance, simulation, focusing, space-charge 3339
 
  • T. Kikuchi
  • K. Horioka
    TIT, Yokohama
  • S. Kawata
    Utsunomiya University, Utsunomiya
  Funding: This work is supported by MEXT (Ministry of Education, Culture, Sports, Science and Technology) and JSPS (Japan Society for the Promotion of Science) No.17740361.

For researches in high energy density physics and inertial confinement fusion by using heavy ion beams, high-current beam dynamics should be understood well. The heavy ion beam is longitudinally compressed by a head-to-tail velocity tilt applied from high-power induction voltage modules. In this study, emittance growth due to the longitudinal bunch compression is numerically investigated by using a particle-in-cell simulation. The code developed is dealt with three dimensional particle motions, and 2D transverse electric field is solved by Poisson equation coupled with 1D longitudinal electric field. We indicate the particle dynamics due to the non-linear longitudinal-transverse coupling effect around the stagnation point in the longitudinal compression.

 
 
THPAN083 A Beam-Slice Algorithm for Transport Simulations of the DARHT-2 Accelerator simulation, emittance, extraction, target 3411
 
  • C. H. Thoma
  • T. P. Hughes
    Voss Scientific, Albuquerque, New Mexico
  A beam-slice algorithm has been implemented into the Lsp particle-in-cell (PIC) code to allow for efficient simulation of beam electron transport through a long accelerator. The slice algorithm pushes beam particles along a virtual axial dimension and performs a field solve on a transverse grid which moves with the particle slice. Any external electric and magnetic fields are also applied to the slice at each time step. For an axisymmetric beam problem the slice algorithm is very fast compared to full 2-D r-z PIC simulations. The algorithm also calculates beam emittance growth due to mismatch oscillations, in contrast to standard envelope codes which assume constant emittance. Using the slice algorithm we are able to simulate beam transport in the DARHT-2 accelerator at LANL from the region just downstream of the diode to the end of the accelerator, a distance of about 50 meters. Results from the slice simulation are compared to both 2-D PIC simulations and the beam envelope code Lamda. The sensitivity of the final emittance to imperfect tuning of the transport solenoids is calculated.  
 
THPAS073 Simplified Charged Particle Beam Transport Modeling Using Commonly Available Commercial Software emittance, controls, optics, lattice 3651
 
  • D. Douglas
  • K. Beard, J. Eldred, P. Evtushenko, A. Jenkins, S. W. Moore, L. Osborne, D. W. Sexton, C. Tennant
    Jefferson Lab, Newport News, Virginia
  Funding: Supported by the Office of Naval Research, the Joint Technology Office, the Commonwealth of Virginia, the Air Force Research Laboratory, Army Night Vision Lab, and by DOE Contract DE-AC05-060R23177.

Particle beam modeling in accelerators has been the focus of much effort (at great expense) since the 1950s. Several generations of tools have resulted from this process, each leveraging both the understanding provided by predecessors and the availability of increasingly powerful computer hardware. Nonetheless, the process remains on-going, in part due to innovations in accelerator design, construction, and operation that result in machines not easily described by existing tools. We discuss a novel response to this issue, which was encountered when Jefferson Lab began operation of its energy-recovering linacs. As such machines are not conveniently described using legacy software, a machine model was been built using Microsoft Excel. This interactive simulation can query data from the accelerator, use it to compute machine parameters, analyze difference orbit data, and evaluate beam properties. It can also derive new accelerator tunings and rapidly evaluate the impact of changes in machine configuration. As it is spreadsheet-based, it can be easily user-modified in response to changing requirements. Examples for the JLab IR Upgrade FEL are presented.

 
 
THPAS102 Uniform Beam Distributions at the Target of the NSRL Beam Transfer Line target, ion, octupole, booster 3720
 
  • N. Tsoupas
  • L. Ahrens, K. A. Brown, I.-H. Chiang, C. J. Gardner, W. W. MacKay, P. H. Pile, A. Rusek
    BNL, Upton, Long Island, New York
  Funding: Work supported by the US Department of Energy

Uniform irradiation of biological or material samples with charged particle beams is desired by experimentalist because it reduces radiation-dose-errors which are introduced by a non-uniform irradiation of the samples. In this paper we present results of uniform beams produced in the NASA SPACE RADIATION LABORATORY (NSRL) at the Brookhaven National Laboratory (BNL) by a method which was conceived theoretically and tested experimentally at BNL. This method* of producing uniform beams in the transverse beam direction, is based on purely magnetic focusing of the beam and requires no collimation of the beam or any other type of beam interaction with materials. The method is favorably compared with alternative methods** of producing uniform beam distributions normal to the beam direction and can be applied to the whole energy spectrum of the charged particle beams that are delivered by the Booster synchrotron at BNL.

*Uniform Particle Beam Distribution Produced by Octupole Focusing N. Tsoupas et. al. NSE: 126, 71-79 (1997)
**Review of Ion Beam Therapy: Present and Future J. Alonso LBNL EPAC 2000

 
 
FRPMN008 Wave Breaking and Particle Jets in Inhomogeneous Beams emittance, simulation, focusing, plasma 3886
 
  • R. P. Nunes
  • Y. Levin, R. Pakter, F. B. Rizzato
    IF-UFRGS, Porto Alegre
  Funding: CNPq, Brasil and AFOSR under grant FA9550-06-1-0345.

We analyze the dynamics of inhomogeneous, magnetically focused high-intensity beams of charged particles. While for homogeneous beams the whole system oscillates with a single frequency, any inhomogeneity leads to propagating transverse density waves which eventually result in a singular density build up, causing wave breaking and jet formation. The theory presented in this paper allows to analytically calculate the time at which the wave breaking takes place. It also gives a good estimate of the time necessary for the beam to relax into the final stationary state consisting of a cold core surrounded by a halo of highly energetic particles.

 
 
FRPMS054 PSR Electron Cloud Detector and Suppressor Mechanical Design and Fabrication electron, quadrupole, vacuum, diagnostics 4117
 
  • J. F. O'Hara
  • M. J. Borden, A. A. Browman, N. A. Gillespie, D. Martinez, K. G. McKeown, F. R. Olivas
    LANL, Los Alamos, New Mexico
  • J. E. Ledford, R. J. Macek
    TechSource, Santa Fe, New Mexico
  Funding: Work supported by DOE SBIR Grant No. DE-FG02-04ER84105 and CRADA No. LA05C10535 between TechSource, Inc. and the Los Alamos National Laboratory.

In order to better understand the two stream e-p instability issue in the LANSCE Proton Storage Ring, a new diagnostic instrument has been developed to measure the electron cloud formation and trapping in a quadrupole magnet at the LANSCE, PSR. The device called the Electron Cloud Detector (ECD) was fabricated and has successfully been installed in the PSR. Along with the Electron Cloud Detector, an additional device was developed to manipulate electrons ejected from the quadrupole and allow additional information to be obtained from ECD measurements. This paper will discuss the mechanical design and fabrication issues encountered during the course of developing both devices.