Paper |
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Other Keywords |
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MOXBCH01 |
Industrial Technology for Unprecendented Energy and Luminosity: the Large Hadron Collider
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hadron, vacuum, cryogenics |
6 |
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- P. Lebrun
CERN, Geneva
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With over 2.7 billion Swiss francs procurement contracts under execution in industry and the installation of major technical systems proceeding in its first 3.3 km sector, the Large Hadron Collider (LHC) construction is now in full swing at CERN, the European Organization for Nuclear Research. The LHC is not only the most challenging particle accelerator under construction, it is also the largest global project ever for a scientific instrument based on advanced technology. Starting from accelerator performance requirements, we recall how these can be met by an appropriate combination of technologies, such as high-field superconducting magnets, superfluid helium cryogenics, beam and insulation vacuum or power electronics, with particular emphasis on the developments required to meet demanding specifications, and the industrialization issues which had to be solved for achieving series production of precision components under tight quality assurance and within limited resources. This provides the opportunity for reviewing the production status of the different systems and the progress of the project.
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Video of talk
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Transparencies
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MOYCH01 |
The TESLA XFEL Project
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linac, hadron, vacuum, cryogenics |
11 |
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MOYCH02 |
Physics Challenges for ERL Light Sources
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hadron, extraction, vacuum, cryogenics |
16 |
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- L. Merminga
Jefferson Lab, Newport News, Virginia
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We present an overview of the physics challenges encountered in the design and operation of Energy Recovering Linac (ERL) based light sources. These challenges include the generation and preservation of low emittance, high-average current beams, manipulating and preserving the transverse and longitudinal phase space, control of the multipass beam breakup instability, efficient extraction of higher order mode power and RF control and stability of the superconducting cavities. These key R&D issues drive the design and technology choices for proposed ERL light sources. Simulations and calculations of these processes will be presented and compared with experimental data obtained at the Jefferson Lab FEL Upgrade, a 10 mA ERL light source presently in commissioning, and during a 1 GeV demonstration of energy recovery at CEBAF.
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Video of talk
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Transparencies
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MOZCH01 |
Technologies for Electron-positron Linear Colliders
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damping, synchrotron, extraction, impedance |
26 |
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MOZCH02 |
Start to End Simulations of Low Emittance Tuning and Stabilization
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simulation, emittance, synchrotron, damping |
31 |
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- P. Tenenbaum, A. Seryi, M. Woodley
SLAC, Menlo Park, California
- D. Schulte
CERN, Geneva
- N.J. Walker
DESY, Hamburg
- G.R. White
Queen Mary University of London, London
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The principal beam dynamics challenge to the subsystems between the damping ring and the collision point of future linear colliders is expected to be the tuning and stabilization required to preserve the transverse emittance and to collide nanometer-scale beams. Recent efforts have focused on realistically modelling the operation and tuning of this region, dubbed the Low Emittance Transport (LET). We report on the development of simulation codes which permit integrated simulation of this complex region, and on early results of these simulations. Future directions of LET simulation are also revealed.
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Video of talk
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Transparencies
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WEPLT169 |
Benchmark and Threshold Analysis of Longitudinal Microwave Instability in the PSR
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electron, sextupole, optics, wakefield |
2221 |
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- S.M. Cousineau, J.A. Holmes
ORNL/SNS, Oak Ridge, Tennessee
- C. Beltran, R.J. Macek
LANL/LANSCE, Los Alamos, New Mexico
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A set of inductive inserts used to provide passive longitudinal space charge compensation in the Los Alamos Proton Storage Ring cause a strong microwave instability in the beam when the inductors are at room temperature. We use the ORBIT code to perform benchmarks of the microwave instability dynamics, including the mode spectrum and the instability growth time. Additionally, we analyze the experimental instability intensity threshold and compare it with the simulated threshold. For all parameters benchmarked, results of simulations are in good agreement with the experimental data.
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WEPLT170 |
Injection Schemes for Self Consistent Space Charge Distributions
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electron, sextupole, optics, wakefield |
2224 |
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- V.V. Danilov, S.M. Cousineau, S. Henderson, J.A. Holmes, M. Plum
ORNL/SNS, Oak Ridge, Tennessee
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This paper is based on recently found sets of self-consistent 2D and 3D time-dependent space charge distributions. A subset of these distributions can be injection-painted into an accumulator ring, such as Spallation Neutron Source Ring, to produce periodic space charge conditions. The periodic condition guarantees zero space-charge-induced halo growth and beam loss during injection. Practical aspects of such schemes are discussed, and simulations of a few specific cases are presented.
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WEPLT171 |
Rotating Electromagnetic Field Trap for High Temperature Plasma and Charge Confinement
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electron, sextupole, optics, wakefield |
2227 |
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- V.V. Danilov
ORNL/SNS, Oak Ridge, Tennessee
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This paper demonstrates that there exists a special combination of oscillating electromagnetic fields capable of trapping ultra high charge densities. Trapped particles undergo stable motion when their frequencies of oscillation are much higher than that of the ocillating field. Contrary to conventional electromagnetic traps, the motion in this dynamic trap is stable for arbitrarily high electromagnetic field amplitudes. This, in turn, leads to the possibility of using enormous electric and magnetic fields from RF or laser sources to confine dense ultrahigh temperature plasmas and particle beams.
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WEPLT172 |
Design & Handling of High Activity Collimators &Ring Components on the SNS
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electron, sextupole, optics, wakefield |
2230 |
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- G.R. Murdoch, D. Crisp, S. Henderson, M. Holding, K. Potter, T. Roseberry
ORNL/SNS, Oak Ridge, Tennessee
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Design & Handling of High Activity Collimators on the SNS*G Murdoch,S Henderson, K Potter,T Roseberry,Oak Ridge National Laboratory, USA,H Ludewig, N Simos, Brookhaven National Laboratory, USAJ Hirst, Rutherford Appleton Laboratory,UK, The Spallation Neutron Source accelerator systems will provide a 1GeV, 1.44MW proton beam to a liquid mercury target for neutron production. The expected highest doses to components are in the collimator regions. This paper presents the mechanical engineering design of a typical collimator highlighting the design features incorporated to assist with removal once it is activated. These features include shielding and lifting fixtures but more importantly a double contained flexible water system incorporating remote water couplings.Also presented is a mechanism that allows axial removal of vacuum bellows and its associated vacuum clamps.*SNS is managed by UT-Battelle, LLC, under contract DE-AC05-00OR22725 for the U.S. Department of Energy. SNS is a partnership of six national laboratories: Argonne, Brookhaven, Jefferson, Lawrence Berkeley, Los Alamos and Oak Ridge.
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WEPLT174 |
Higher Order Hard Edge End Field Effects
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electron, sextupole, optics, wakefield |
2233 |
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- J.S. Berg
BNL, Upton, Long Island, New York
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In most cases, nonlinearities from magnets must be properly included in tracking and analysis to properly compute quantities of interest, in particular chromatic properties and dynamic aperture. One source of nonlinearities in magnets that is often important and cannot be avoided is the nonlinearity arising at the end of a magnet due to the longitudinal variation of the field at the end of the magnet. Part of this effect is independent of the shape of the end. It is lowest order in the body field of the magnet, and is the result of taking a limit as the length over which the field at the end varies approaches zero. This is referred to as a hard edge" end field. This effect has been computed previously to lowest order in the transverse variables. This paper describes a method to compute this effect to arbitrary order in the transverse variables, under certain constraints. The results of using this hard edge model are compared with performing the computation with finite-length end fields, as well as to the lowest-order hard-edge end field model.
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WEPLT177 |
Analysis of Electron Cloud at RHIC
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sextupole, optics, wakefield, electron |
2236 |
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- U. Iriso, M. Blaskiewicz, P. Cameron, K.A. Drees, W. Fischer, H.-C. Hseuh, R. Lee, S. Peggs, L. Smart, D. Trbojevic, S.Y. Zhang
BNL, Upton, Long Island, New York
- G. Rumolo
GSI, Darmstadt
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Pressure rises with high intense beams are becoming the main luminosity limitation at RHIC. Observations during the latest runs show beam induced electron multipacting as one of the causes for these pressure rises. Experimental studies are carried out at RHIC using devoted instrumentation to understand the mechanism leading to electron clouds. Possible cures using NEG coated beam pipes and solenoids are experimentally tested. In the following, we report the experimental electron cloud data and analyzed the results using computer simulation codes.
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WEPLT181 |
Measurement of Multipole Strengths from RHIC BPM Data
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sextupole, optics, wakefield, electron |
2239 |
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WEPLT182 |
Non-linear Modeling of the RHIC Interaction Regions
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sextupole, optics, wakefield, electron |
2242 |
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- R. Tomas, W. Fischer, A.K. Jain, Y. Luo, F.C. Pilat
BNL, Upton, Long Island, New York
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For RHIC's collision lattices the dominant sources of transverse non-linearities are located in the interaction regions. The field quality is available for most of the magnets in the interaction regions from the magnetic measurements, or from extrapolations of these measurements. We discuss the implementation of these measurements on the MADX models of the Blue and the Yellow rings and their impact on beam stability.
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WEPLT183 |
Clearing of Electron Cloud in SNS
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sextupole, optics, wakefield, beamloading |
2245 |
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- L. Wang, Y.Y. Lee, D. Raparia, J. Wei, S.Y. Zhang
BNL, Upton, Long Island, New York
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In this paper we describe a mechanism using the clearing electrodes to remove the electron cloud in the Spallation Neutron Source (SNS) accumulator ring, where strong multipacting could happen at median clearing fields. A similar phenomenon was reported in an experimental study at Los Alamos laboratory's Proton Synchrotron Ring (PSR). We also investigated the effectiveness of the solenoid's clearing mechanism in the SNS, which differs from the short bunch case, such as in B-factories.
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WEPLT184 |
Preliminary Estimation of the Electron Cloud in RHIC
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sextupole, optics, wakefield, electron |
2248 |
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THXCH01 |
Achieving Sub-micron Stability in Light Sources
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sextupole, optics, wakefield, beamloading |
211 |
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- M. Böge
PSI, Villigen
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One of the major goals for present and future light sources is to achieve sub-micron orbit stability of the electron beam at the photon beam source points over a large frequency range. This puts tight constraints on the design of the various accelerator components like girders, magnets, power supplies and diagnostic hardware. Fast orbit feedbacks systems based on high performance RF- and X-BPMs become essential to suppress residual orbit distortions. Furthermore the "top-up" operation mode which guaranties a constant electron beam current and thus a constant heat load in 3rd generation light sources is one of the key ingredients to reach sub-micron stability.
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Video of talk
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Transparencies
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THOACH01 |
SPEAR3 Commissioning
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sextupole, wakefield, beamloading, beamlosses |
216 |
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- J.A. Safranek, S. Allison, P. Bellomo, W.J. Corbett, M. Cornacchia, E. Guerra, R.O. Hettel, D. Keeley, N. Kurita, D.J. Martin, P.A. McIntosh, H. Morales, G.J. Portmann, F.S. Rafael, H. Rarback, J.J. Sebek, T. Straumann, A. Terebilo, J. Wachter, C. Wermelskirchen, M. Widmeyer, R. Yotam
SLAC/SSRL, Menlo Park, California
- M.J. Boland, Y.E. Tan
ASP, Melbourne
- J.M. Byrd, D. Robin, T. Scarvie, C. Steier
LBNL/ALS, Berkeley, California
- M. Böge
PSI, Villigen
- H.-P. Chang, C.-C. Kuo, H.-J. Tsai
NSRRC, Hsinchu
- W. Decking
DESY, Hamburg
- M.G. Fedurin, P. Jines
LSU/CAMD, Baton Rouge, Louisiana
- K. Harkay, V. Sajaev
ANL/APS, Argonne, Illinois
- S. Krinsky, B. Podobedov
BNL/NSLS, Upton, Long Island, New York
- L.S. Nadolski
SOLEIL, Gif-sur-Yvette
- A. Ropert
ESRF, Grenoble
- M. Yoon
POSTECH, Pohang, Kyungbuk
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Starting in April, 2003, the SPEAR2 storage ring was removed and replaced with a new 500 mA, 3 GeV light source, SPEAR3. The SPEAR2 storage ring had been in use for high energy physics, then synchrotron radiation since 1972. Commissioning of SPEAR3 started on December 8, 2003 and synchrotron radiation will be delivered to the first users on March 8, 2004. SPEAR3 commissioning will be reviewed, including discussion of diagnostics, orbit control, optics correction and high current studies.
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Video of talk
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Transparencies
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THOACH02 |
Commissioning of the 500 MeV Injector for MAX-lab
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sextupole, wakefield, beamloading, beamlosses |
219 |
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- S. Werin, Å. Andersson, M. Bergqvist, M. Brandin, M. Demirkan, M. Eriksson, L.-J. Lindgren, L. Malmgren, H. Tarawneh, E.J. Wallén
MAX-lab, Lund
- B. Anderberg
AMACC, Uppsala
- G. Georgsson
Danfysik A/S, Jyllinge
- G. LeBlanc
ASP, Melbourne
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A 500 MeV new injector system for the storage rings MAX I, II and III have been installed during the winter 2003-4 at MAX-lab. The system consists of two linacs at 125 MeV each, using SLED, and a recirculating system such that the electrons pass the linacs twice, thus reaching a final energy of 500 MeV. The system is injected by a thermionic RF-gun. The commissioning of the complete system will be performed in the spring 2004.
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Video of talk
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Transparencies
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THOACH03 |
Top-up Operation at SPring-8 - Towards Maximizing the Potential of a 3rd Generation Light Source
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injection, wakefield, beamloading, beamlosses |
222 |
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- H. Tanaka, T. Aoki, T. Asaka, S. Daté, K. Fukami, Y. Furukawa, H. Hanaki, N. Hosoda, T. Kobayashi, N. Kumagai, M. Masaki, T. Masuda, S. Matsui, A. Mizuno, T. Nakamura, T. Nakatani, T. Noda, T. Ohata, H. Ohkuma, T. Ohshima, M. Oishi, S. Sasaki, J. Schimizu, M. Shoji, K. Soutome, M. Suzuki, S. Suzuki, S. Takano, M. Takao, T. Takashima, H. Takebe, K. Tamura, R. Tanaka, T. Taniuchi, Y. Taniuchi, K. Tsumaki, A. Yamashita, K. Yanagida, H. Yonehara, T. Yorita
JASRI/SPring-8, Hyogo
- M. Adachi, K. Kobayashi, M. Yoshioka
SES, Hyogo-pref.
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Top-up operation maximizes research activities in a light source facility by an infinite beam lifetime and photon beam stability. We have been improving the SPring-8 accelerators to achieve the ideal top-up operation. For the perturbation-free injection, we adjusted the magnetic field shape of four bump magnets to close the bump orbit, and introduced a scheme to suppress the stored beam oscillation induced by the nonlinearlity of sextupole magnets. These reduced the horizontal oscillation down to a third of the stored beam size. For the loss-free injection, beam collimators were installed upstream of the injection line. This realized the injection efficiency of ~100% under the restricted gap condition of in-vacuum insertion devices (ID). Since autumn 2003, we have been injecting the beams keeping the photon beam shutters opened and ID gaps closed. We developed a bunch-by-bunch feedback system to reduce the beam loss further with all the ID gaps fully closed by lowering the operating chromaticity. The operation with constant stored current is scheduled in June 2004. We present the overview and progress of the SPring-8 top-up operation focusing on our developments and results.
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Video of talk
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Transparencies
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THYCH01 |
Issues and Challenges for Short Pulse Radiation Production
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electron, injection, wakefield, beamloading |
225 |
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- P. Emma
SLAC/ARDA, Menlo Park, California
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A new generation of light sources are being planned at many locations, pushing the frontiers of brightness, wavelength, and peak power well beyond existing 3rd generation sources. In addition to these large scale improvements there is great interest in extremely short duration pulses into the femtosecond and sub-femtosecond regime. Collective electron bunch instabilities at these scales are severe, especially in consideration of the high-brightness electron bunch requirements. Several new schemes propose very short radiation pulses generated with moderate electron bunch lengths. Such schemes include radiation pulse compression, differential bunch spoiling, staged high-gain harmonic generation, and selective pulse seeding schemes. We will describe a few of these ideas and address some of the electron bunch length limitations, highlighting recent measurements at the Sub-Picosecond Pulse Source (SPPS) at SLAC where <100-fs electron and x-ray pulses are now available.
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Video of talk
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Transparencies
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THOBCH01 |
The Beijing Electron-positron Collider and its Second Phase Construction
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synchrotron, injection, radiation, wakefield |
230 |
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- C. Zhang, J.Q. Wang
IHEP Beijing, Beijing
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The Beijing Electron-Positron Collider (BEPC) was constructed for both high energy physics and synchrotron radiation researches. As an e+e- collider operating in the tau-charm region and a first synchrotron radiation source in China, the machine has been well operated for 14 years since it was put into operation in 1989. As a collider, the peak luminosity of the BEPC has reached its design goal of 5*1030 cm-2s-1 at J/sai energy of 1.55 GeV and 1*1031 cm-2s-1 at 2 GeV respectively. The main parameters in the dedicated synchrotron radiation operation are: E=2.2~2.5 GeV, ex0=80 mm mrad at 2.2 GeV, Ib=140 mA and the beam lifetime of 20~30 hours. As the second phase project of the BEPC, the BEPCII , has been approved with total budget of 640 million RMB. The construction is started in the beginning of 2004 and is scheduled to complete by the end of 2007. The BEPCII is a double ring machine with its luminosity goal of 1*1033 cm-2s-1 at 1.89 GeV, two orders of magnitude higher than present BEPC. The BEPCII will operate in the beam energy of 1-2.1 GeV so that its physical potential in the whole t and charm range is preserved, while the collider will be optimized at 1.89 GeV. The upgrading of the collider should also provide an improved SR performance with higher beam energy and intensity. The beam currents will be increased to 250 mA at E=2.5 GeV for the dedicated synchrotron radiation operation of the BEPCII. Some key technologies, such as superconducting RF system, low impedance vacuum devices, superconducting micro-beta quadrupoles and etc., has been intensively studied in order to achieve the target of the BEPCII.
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Video of talk
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Transparencies
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