SLAC实验的螺旋相关系统

P. Mastromarino, T. Humensky, P. Anthony, C. Arroyo, K. Bega, A. Brachmann, G. Cates, J. Clendenin, F. Decker, T. Fieguth, E. Hughes, G. M. Jones, Y. Kolomensky, K. Kumar, D. Relyea, S. Rock, O. Saxton, Z. Szalata, J. Turner, M. Woods
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引用次数: 5

摘要

在SLAC上的E158实验将首次测量Moller散射中的宇称破坏。45 GeV极化电子束与非极化电子在液氢靶中的弹性散射的左右横截面不对称性测量精度优于10/sup -8/,期望的标准模型不对称性约为10/sup -7/。由于电子束中螺旋相关(左右)电荷和位置的不对称性会在测量中引起系统误差,因此必须非常注意电子束的监测和控制。我们开发了光束电流监测器,以3 /spl次/ 10/sup -5/电平测量每脉冲的电荷,射频腔光束位置监测器测量每脉冲的位置到1 /spl mu/m,这应该允许最终集成电荷和位置不对称的精度分别为1 ppb和1 nm。此外,由于电子束中大多数与螺旋度相关的系统学可以追溯到驱动砷化镓源阴极光发射的激光,我们首先使用仔细控制激光束偏振,点对点成像和其他技术来最小化系统学。我们还提供了以螺旋相关方式调制激光束照射到光电阴极时的强度和位置的能力,允许实现主动反馈,以确保在实验过程中平均电荷和位置不对称的积分接近于零。我们介绍了这个精密光束监测和控制系统,并报告了其在SLAC最近的调试运行中的性能,T-437,其电荷和位置不对称精度分别为2 ppb和12 nm。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Helicity-correlated systematics for SLAC Experiment E158
Experiment E158 at SLAC will make the first measurement of parity violation in Moller scattering. The left-right cross-section asymmetry in the elastic scattering of a 45 GeV polarized electron beam with unpolarized electrons in a liquid hydrogen target will be measured to an accuracy of better than 10/sup -8/, with the expected Standard Model asymmetry being approximately 10/sup -7/. Because helicity-correlated (left-right) charge and position asymmetries in the electron beam can give rise to systematic errors in the measurement, great care must be given to beam monitoring and control. We have developed beam current monitors that measure the charge per pulse at the 3 /spl times/ 10/sup -5/ level and RF cavity beam position monitors that measure the position per pulse to 1 /spl mu/m, which should allow precisions of 1 ppb and 1 nm for the final integrated charge and position asymmetries, respectively. In addition, since most helicity-correlated systematics in the electron beam can be traced back to the laser that drives the photoemission from the GaAs source cathode, we first use careful control of laser beam polarization, point-to-point imaging, and other techniques to minimize systematics. We also provide the capability of modulating in a helicity-correlated way the laser beam's intensity and position as it strikes the photocathode, allowing the implementation of active feedback to ensure that the average charge and position asymmetries integrate close to zero over the course of the experiment. We present this system of precision beam monitoring and control and report on its performance during a recent commissioning run, T-437 at SLAC, which demonstrated charge and position asymmetry precision of 2 ppb and 12 nm, respectively.
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