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References - Bogoliubov Laboratory of Theoretical Physics - JINR

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PROTON BEAM POLARIZATION MEASUREMENTS AT RHIC<br />

A. Bazilevsky 1 , I. Alekseev 2 , E. Aschenauer 1 ,G.Atoyan 1 ,A.Bravar 3 ,G.Bunce 1 ,<br />

G. Boyle 4 ,C.M.Camacho 5 , V. Dharmawardane 6 , R. Gill 1 , H. Huang 1 ,S.Lee 7 ,X.Li 8 ,<br />

H. Liu 6 ,Y.Makdisi 1 , B. Morozov 1 , I. Nakagawa 4,9 ,H.Okada 1 ,D.Svirida 2 ,<br />

M. Sivertz 1 and A. Zelenski 1<br />

(1) Brookhaven National <strong>Laboratory</strong>, Upton, NY 11973, USA<br />

(2) Institute for <strong>Theoretical</strong> and Experimental <strong>Physics</strong> (ITEP), 117259 Moscow, Russia<br />

(3) University <strong>of</strong> Geneva, 1205 Geneva, Switzerland<br />

(4) RIKEN-BNL Research Center, Upton, NY 11973, USA<br />

(5) Los Alamos National <strong>Laboratory</strong>, Los Alamos, NM 87545, USA<br />

(6) New Mexico State University, Las Cruces, NM 88003, USA<br />

(7) Stony Brook University, SUNY, Stony Brook, NY 11794, USA<br />

(8) Shandong University, China<br />

(9) RIKEN, 2-1 Hirosawa Wako, Saitama 351-0198, Japan<br />

Abstract<br />

We discuss the beam polarization measurement strategy at RHIC with achieved<br />

relative precision <strong>of</strong> better than 5%.<br />

1 Introduction<br />

Polarimetry is one <strong>of</strong> the crucial part <strong>of</strong> the RHIC Spin Program [1]. It provides precise<br />

measurements <strong>of</strong> beam polarizations which is a necessary component <strong>of</strong> all high precision<br />

spin dependent measurements at RHIC.<br />

Two types <strong>of</strong> polarimeters are used at RHIC, which are based on small angle elastic<br />

scattering, with sensitivity to the proton beam polarization coming from interference<br />

between electromagnetic and hadronic amplitudes (Coulomb-Nuclear Interference (CNI)<br />

region).<br />

One type <strong>of</strong> polarimeter (pC) uses an ultra-thin (10–20 μg/cm 2 ) carbon ribbon target,<br />

and provides fast relative polarization measurements with a few percent statistical<br />

uncertainty in 20–30 sec. The other type polarimeter (H-Jet) uses a polarized hydrogen<br />

gas target and utilizes the analyzing power in proton-proton elastic scattering in the<br />

CNI region. It accumulates data over the entire store and provides absolute polarization<br />

measurements, with ∼10% statistical uncertainty in a store (6–8 hours). H-Jet data accumulated<br />

over several stores are used for the absolute calibration <strong>of</strong> the pC polarimeters.<br />

In addition, two experiments STAR and PHENIX employ local polarimeters which<br />

are used to set up and to monitor the spin direction at collision. They also proved to be<br />

a valuable tool for beam polarization monitoring when spin orientation at collision was<br />

set up to be transverse.<br />

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