Accelerating polarized protons to 250 GeV

Mei Bai ,N Tsoupas,G Ganetis,A Marusic,D N Svirida,M Wilinski,J Delong,G Bunce,M Blaskiewicz,A Bravar,P Cameron,A Drees,B Oerter,F Pilat,A Zaltsman,J Piacentino,K Zeno,C Montag,G Marr,T Roser,W W Mackay,T Satogata,S Tepikian,A Zelenski,K Brown,A Luccio,D Bruno,J Butler,R Lee,P Oddo,P Ingrassia,J Alessi,Y Luo,R Connolly,L Ahrens,H Huang,Kevin S Smith ,Y I Makdisi ,John Morris ,H.c Hseuh ,I Alekseev ,J.w Glenn ,T D’ottavio ,G Mclntyre ,D Trbojević ,J.m Brennan ,M.w Fischer ,J Beebe‐Wang ,J Tuozzolo,C Gardner,V Ptitsyn,R Michnoff,T Hayes,J Laster,S.y Zhang

doi:10.1109/pac.2007.4440761

Abstract

The relativistic heavy ion collider (RHIC) as the first high energy polarized proton collider was designed to provide polarized proton collisions at a maximum beam energy of 250 GeV. It has been providing collisions at a beam energy of 100 GeV since 2001. Equipped with two full Siberian snakes in each ring, polarization is preserved during the acceleration from injection to 100 GeV with careful control of the betatron tunes and the vertical orbit distortions. However, the intrinsic spin resonances beyond 100 GeV are about a factor of two stronger than those below 100 GeV making it important to examine the impact of these strong intrinsic spin resonances on polarization survival and the tolerance for vertical orbit distortions. Polarized protons were accelerated to the record energy of 250 GeV in RHIC with a polarization of 46% measured at top energy in 2006. The polarization measurement as a function of beam energy also shows some polarization loss around 136 GeV, the first strong intrinsic resonance above 100 GeV. This paper presents the results and discusses the sensitivity of the polarization survival to orbit distortions.

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