| Paper |
Title |
Page |
| TUPCH105 |
Performance of a Nanometer Resolution BPM System
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1256 |
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- S. Walston, C.C. Chung, P. Fitsos, J.G. Gronberg
LLNL, Livermore, California
- S.T. Boogert
Royal Holloway, University of London, Surrey
- J.C. Frisch, J. May, D.J. McCormick, M.C. Ross, S. Smith, T.J. Smith
SLAC, Menlo Park, California
- H. Hayano, Y. Honda, N. Terunuma, J. Urakawa
KEK, Ibaraki
- Y.K. Kolomensky, T. Orimoto
UCB, Berkeley, California
- A. Lyapin, S. Malton, D.J. Miller
UCL, London
- R. Meller
Cornell University, Department of Physics, Ithaca, New York
- M. Slater, M.T. Thomson, D.R. Ward
University of Cambridge, Cambridge
- V.V. Vogel
DESY, Hamburg
- G.R. White
OXFORDphysics, Oxford, Oxon
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International Linear Collider (ILC) interaction region beam sizes and component position stability requirements will be as small as a few nanometers. It is important to the ILC design effort to demonstrate that these tolerances can be achieved – ideally using beam-based stability measurements. It has been estimated that RF cavity beam position monitors (BPMs) could provide position measurement resolutions of less than one nanometer and could form the basis of the desired beam-based stability measurement. We have developed a high resolution RF cavity BPM system. A triplet of these BPMs has been installed in the extraction line of the KEK Accelerator Test Facility (ATF) for testing with its ultra-low emittance beam. The three BPMs are rigidly mounted inside an alignment frame on variable-length struts which allow movement in position and angle. We have developed novel methods for extracting the position and tilt information from the BPM signals including a calibration algorithm which is immune to beam jitter. To date, we have been able to demonstrate a resolution of approximately 20 nm over a dynamic range of ± 20 microns. We report on the progress of these ongoing tests.
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| WEPLS060 |
CLIC Polarized Positron Source Based on Laser Compton Scattering
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2520 |
| |
- F. Zimmermann, H.-H. Braun, M. Korostelev, L. Rinolfi, D. Schulte
CERN, Geneva
- S. Araki, Y. Higashi, Y. Honda, Y. Kurihara, M. Kuriki, T. Okugi, T. Omori, T. Taniguchi, N. Terunuma, J. Urakawa
KEK, Ibaraki
- X. Artru, R. Chehab, M. Chevallier
IN2P3 IPNL, Villeurbanne
- E.V. Bulyak, P. Gladkikh
NSC/KIPT, Kharkov
- M.K. Fukuda, K. Hirano, M. Takano
NIRS, Chiba-shi
- J. Gao
IHEP Beijing, Beijing
- S. Guiducci, P. Raimondi
INFN/LNF, Frascati (Roma)
- T. Hirose, K. Sakaue, M. Washio
RISE, Tokyo
- K. Moenig
DESY Zeuthen, Zeuthen
- H.D. Sato
HU/AdSM, Higashi-Hiroshima
- V. Soskov
LPI, Moscow
- V.M. Strakhovenko
BINP SB RAS, Novosibirsk
- T. Takahashi
Hiroshima University, Higashi-Hiroshima
- A. Tsunemi
SHI, Tokyo
- V. Variola, Z.F. Zomer
LAL, Orsay
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We describe the possible layout and parameters of a polarized positron source for CLIC, where the positrons are produced from polarized gamma rays created by Compton scattering of a 1.3-GeV electron beam off a YAG laser. This scheme is very energy effective using high finesse laser cavities in conjunction with an electron storage ring. We point out the differences with respect to a similar system proposed for the ILC.
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| THPCH154 |
Development of Pulsed Laser Super-cavity for Compact High Flux X-ray Sources
|
3155 |
| |
- K. Sakaue, M. Washio
RISE, Tokyo
- S. Araki, Y. Higashi, Y. Honda, T. Taniguchi, J. Urakawa
KEK, Ibaraki
- M.K. Fukuda, M. Takano
NIRS, Chiba-shi
- H. Sakai
ISSP/SRL, Chiba
- N. Sasao
Kyoto University, Kyoto
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Pulsed-laser super-cavity is being developed at KEK-ATF for the application of a compact high brightness x-ray source based on Laser Compton Scattering. We use a Fabry-Perot optical cavity with a pulsed laser. The cavity increases a laser effective power, and at the same time, stably makes a small laser spot in side the cavity. In addition, the pulsed-laser gives much higher peak power. Thus, this scheme will open up a new possibility for building a compact high-brightness x-ray source, when collided with an intense bunched electron beam. We are now planning to build such an x-ray source with a 50MeV multi-bunch linac and a 42cm Fabry-Perot cavity using pulse stacking technology. We actually finished construction of the 50MeV linac and will start its operation in the spring, 2006. Development of the pulsed-laser super-cavity and future plan of our compact x-ray source will be presented at the conference.
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