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Etude de la faisabilité d'une source de positrons polarisée basée sur ...

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tel-00647307, version 1 - 1 Dec 2011<br />

1 Synopsis<br />

The purpose of this letter is to inform, and seek approval from, the Program<br />

Advisory Committee for an experiment we would like to perform during the<br />

6-month shutdown (May-October, 2011) for the 12 GeV Upgra<strong>de</strong>. The experiment<br />

constitutes the Ph.D. Thesis of Jonathan Dumas (LPSC/JLab) and<br />

would be the first ever <strong>de</strong>monstration and mea<strong>sur</strong>ement for producing po<strong>la</strong>rized<br />

<strong>positrons</strong> using a po<strong>la</strong>rized electron beam. The experimentis proposed to<br />

occur in the CEBAF injector using a new <strong>de</strong>dicated electronbeam lineand an<br />

experimental apparatus successfully applied at the SLAC E166 experiment[1]<br />

to <strong>de</strong>monstrate po<strong>la</strong>rized <strong>positrons</strong> by an alternative method. The proposed<br />

beam energy for the experiment is 3-8 MeV which can be provi<strong>de</strong>d by the<br />

injector cryounit ( 1<br />

4<br />

cryomodule). The low electron beam current required (1-<br />

10 µA) implies a re<strong>la</strong>tively straight-forward and low-power target conversion<br />

systemandsmall radiationbudget.Thepositron po<strong>la</strong>rizationwillbemea<strong>sur</strong>ed<br />

by a Compton transmission po<strong>la</strong>rimeter. To perform this experiment during<br />

the 6-month shutdown we propose to temporarily segment the lowest MeV<br />

energy region of the injector from the remaining CEBAF complex. This configuration<br />

and long shutdown provi<strong>de</strong> ample time to install the segmentation,<br />

then install, commission and perform the experiment, and finally recover the<br />

original injector configuration in advance of restoring the injector for CEBAF<br />

operations.<br />

2 Motivation<br />

An efficient scheme for positron production, wi<strong>de</strong>ly used in particle accelerators,<br />

relieson thecreationof electron-positron pairsfrom highenergyphotons.<br />

A significant aspect of the process is the <strong>de</strong>pen<strong>de</strong>nce on the po<strong>la</strong>rization, in<br />

particu<strong>la</strong>r, the circu<strong>la</strong>rpo<strong>la</strong>rization of the photon transfers to the longitudinal<br />

po<strong>la</strong>rization of the positron [2]. This is the basic concept of operation tested<br />

for the po<strong>la</strong>rized positron <strong>source</strong> being <strong>de</strong>veloped for the International Linear<br />

Colli<strong>de</strong>r (ILC). The circu<strong>la</strong>rlypo<strong>la</strong>rized photons are produced either from the<br />

Compton back-scatteringof a <strong>la</strong>serlightfrom high energyelectrons[3] or from<br />

the synchrotron radiation of very high energy electrons travelling through a<br />

helical undu<strong>la</strong>tor [1], the <strong>la</strong>tter approach selected for the ILC. This letter of<br />

intent proposes an experiment to investigate an alternative scheme based on<br />

the po<strong>la</strong>rized bremsstralhung process [4].<br />

Simi<strong>la</strong>rly to pair creation, the bremsstrahlung process is a po<strong>la</strong>rization sensitive<br />

mechanism. This property has been wi<strong>de</strong>ly used at un-po<strong>la</strong>rized electron<br />

accelerators to produce linearly po<strong>la</strong>rized photon beams. In addition to the<br />

intrinsic linear po<strong>la</strong>rization, the photons have a circu<strong>la</strong>r component when the<br />

incoming electron beam is po<strong>la</strong>rized, such that the bremsstrahlung of po<strong>la</strong>rized<br />

electrons most generally lead to elliptically po<strong>la</strong>rized photons [2,5]. This<br />

concept is routinely used to obtain a linearly or a circu<strong>la</strong>rly po<strong>la</strong>rized photon<br />

beam at Hall B [6] at several GeV beam energy.<br />

2

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