Compton scattering off polarized electrons with a high-finesse Fabry-Perot Cavity at JLab

被引:34
作者
Falletto, N
Authier, M
Baylac, M
Boyer, M
Bugeon, F
Burtin, E
Cavata, C
Colombel, N
Congretel, G
Coquillard, R
Coulloux, G
Couzy, B
Deck, P
Delbart, A [1 ]
Desforges, D
Donati, A
Duboué, B
Escoffier, S
Farci, F
Frois, B
Girardot, P
Guillotau, J
Henriot, C
Jeanney, C
Juillard, M
Jorda, JP
Legou, P
Lhuillier, D
Lussignol, Y
Mangeot, P
Martin, X
Marie, F
Martino, J
Maurier, M
Mazeau, B
Millot, JF
Molinié, F
Mols, JP
Mouly, JP
Mur, M
Neyret, D
Pédrol, T
Platchkov, S
Pontet, G
Pussieux, T
Queinec, Y
Rebourgeard, P
Sellier, JC
Tarte, G
Veyssière, C
机构
[1] CEA Saclay, DSM, DAPNIA, F-91191 Gif Sur Yvette, France
[2] LPC, IN2P3, Clermont Ferrand, France
[3] Thomas Jefferson Natl Accelerator Facil, Newport News, VA 23606 USA
[4] Univ Lyon 1, IPNL, IN2P3, F-69622 Villeurbanne, France
关键词
D O I
10.1016/S0168-9002(00)01049-4
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
We built and commissioned a new type of Compton polarimeter to measure the electron beam polarization at the Thomas Jefferson National Accelerator Facility (Virginia, USA). The heart of this polarimeter is a high-finesse monolithic Fabry-Perot cavity. Its purpose is to amplify a primary 300 mW laser beam in order to improve the signal to noise ratio of the polarimeter. It is the first time that a high-finesse Fabry-Perot cavity is enclosed in the vacuum of a particle accelerator to monitor the beam polarization by Compton polarimetry. The measured finesse and amplification gain of the cavity are F = 26 000 and G = 7300. The electron beam crosses this high-power photon source at an angle of 23 mrad in the middle of the cavity where the photon beam power density is estimated to be 0.85 MW/cm(2). We have used this facility during the HAPPEX experiment (April-July 1999) and we give a preliminary measurement of Compton scattering asymmetry. (C) 2001 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:412 / 425
页数:14
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