2017年RHIC Run中的HJET偏振计

A. Poblaguev, E. Aschenauer, G. Atoian, K. O. Eyser, H. Huang, Y. Makdisi, W. Schmidke, A. Zelenski, I. Alekseev, D. Svirida
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引用次数: 5

摘要

2004年投入使用的极化原子氢喷射靶(HJET)偏振计是用于测量相对论重离子对撞机(RHIC)中质子束的绝对偏振。将讨论HJET在RHIC Run 2017 (255 GeV质子束)中的性能。所测有效分析功率$\langle A_N\rangle$的长期(1-100天)稳定性为$\sqrt{\langle(\delta\sigma^\mathrm{syst}_{A_N})^2\rangle}/A_N\le0.1\%$。测量$P\sim56\%$的RHIC光束平均偏振的系统误差为$\sigma_P^\mathrm{syst}/P\lesssim0.5\%$。这种测量的统计误差由检测到的$p^\uparrow p^\uparrow$弹性事件的数量来定义,对于8小时的RHIC存储,它通常在$\sigma_P^\mathrm{stat}\approx2\%$。Run 2017期间积累的每束RHIC中大约$10^9$的弹性事件统计数据使我们能够在动量传递范围$0.001<-t<0.020~(\mathrm{GeV}⁄c)^2$内详细研究质子-质子单自旋$A_N (t)$和双自旋$A_{NN}(t)$的分析能力。强子单次$r_5$和双次$r_2$自旋翻转振幅的贡献是孤立的。对非弹性背景$p_\mathrm{beam}^\uparrow+p_\mathrm{target}^\uparrow\rightarrow X+p_\mathrm{target}$的分析使我们能够实验地评估$M_X-m_p\lesssim400\ \mathrm{MeV}$和$t\sim-0.005\ (\mathrm{GeV}⁄c)^2$在这些过程中光束和目标自旋相关的不对称性。在RHIC中3周的Gold-Gold光束中获得的数据使我们能够对$E_\text{Lab}=27.2$\unit{}{\GeV}的$p^\uparrow\mathrm{Au}$分析能力进行高统计测量。
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The HJET polarimeter in RHIC Run 2017
The Polarized Atomic Hydrogen Jet Target (HJET) Polarimeter commissioned in 2004 was designed to measure absolute polarization of proton beams in Relativistic Heavy Ion Collider (RHIC). HJET performance in RHIC Run 2017 (255 GeV proton beams) will be discussed. The long term (1-100 days) stability of the measured effective analyzing power $\langle A_N\rangle$ was found to be $\sqrt{\langle(\delta\sigma^\mathrm{syst}_{A_N})^2\rangle}/A_N\le0.1\%$. The systematic error in measurement of the RHIC beam average polarization of $P\sim56\%$ was evaluated to be $\sigma_P^\mathrm{syst}/P\lesssim0.5\%$. The statistical error in such a measurement is defined by the number of detected $p^\uparrow p^\uparrow$ elastic events and for an 8 hours RHIC store it was typically at $\sigma_P^\mathrm{stat}\approx2\%$. The elastic events statistics of about $10^9$ per RHIC beam accumulated during Run 2017 allowed us to make a detailed study of the proton-proton single-spin $A_N (t)$ and double-spin $A_{NN}(t)$ analyzing powers in the momentum transfer range $0.001<-t<0.020~(\mathrm{GeV}⁄c)^2$. Contributions of the hadronic single $r_5$ and double $r_2$ spin-flip amplitudes were isolated. Analysis of the inelastic background $p_\mathrm{beam}^\uparrow+p_\mathrm{target}^\uparrow\rightarrow X+p_\mathrm{target}$ allowed us to experimentally evaluate the beam and target spin correlated asymmetries in these processes for $M_X-m_p\lesssim400\ \mathrm{MeV}$ and $t\sim-0.005\ (\mathrm{GeV}⁄c)^2$. The data acquired during 3 weeks of Gold-Gold beams in RHIC allowed us to make a high statistics measurement of the $p^\uparrow\mathrm{Au}$ analyzing power at $E_\text{Lab}=27.2$\unit{}{\GeV}.
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