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Particle Accelerator Conference (PAC09), Vancouver : Canada (2009)
The CLIC Positron Sources Based on Compton Schemes
L. Rinolfi1, H.-H. Braun1, Y. Papaphilippou1, D. Schulte1, A. Vivoli1, F. Zimmermann1, F. Antoniou, I.R. Bailey, L. Zang, E.V. Bulyak, P. Gladkikh, R. Chehab2, J.A. Clarke, O. Dadoun3, P. Lepercq3, R. Roux3, A. Variola3, Z.F. Zomer3, W. Gai, W. Liu, T. Kamitani, T. Omori, J. Urakawa, M. Kuriki, H. Monard, I. Pogorelsky, V. Yakimenko, T. Takahashi
(2009)

The CLIC polarized positron source is based on a positron production scheme in which polarized photons are produced by Compton process. Compton backscattering happens in a so-called "Compton ring" where an electron beam of 1.06 GeV interacts with a powerful laser beam amplified in an optical resonator. The circularly-polarized gamma rays are sent on to a target, producing pairs of longitudinally polarized electrons and positrons. An Adiabatic Matching Device maximizes the capture of the positrons. A normal-conducting 2 GHz Linac accelerates the beam up to 2.424 GeV before injection into the Pre-Damping Ring (PDR). The nominal CLIC bunch population is 4.4x10**9 particles per bunch. Since the photon flux coming out from a "Compton ring" is not sufficient to obtain the requested charge, a stacking process is required in the PDR. Another option is to use a "Compton Energy Recovery Linac" where a quasi-continual stacking in the PDR could be achieved. A third option is to use a "Compton Linac" which would not require stacking. We describe the overall scheme as well as advantages and constraints of the three different options.
1 :  CERN - European Organization for Nuclear Research
2 :  IPNL - Institut de Physique Nucléaire de Lyon
3 :  LAL - Laboratoire de l'Accélérateur Linéaire
Physique/Physique/Physique des accélérateurs
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