首页> 外文学位 >Measurement of electroweak asymmetries in vector electron positron scattering at 0.1 less than Q(2) less than 0.4 (GeV/c)(2).
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Measurement of electroweak asymmetries in vector electron positron scattering at 0.1 less than Q(2) less than 0.4 (GeV/c)(2).

机译:在矢量电子正电子散射中以0.1小于Q(2)小于0.4(GeV / c)(2)的方式测量电弱不对称性。

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摘要

This work is based on the first engineering run of the G 0 experiment from October 2002 though January 2003 in Hall C at Jefferson Lab. The G0 experiment will be the first to measure the weak neutral form factors: GEZ( Q2), GMZ( Q2) and GAe( Q2) and to extract the proton's strange form factors: GEs(Q2) and GMs(Q 2) via a Rosenbluth separation over a range of Q 2 (0.1--1.0 (GeV/c)2). This will require four sets of measurements: forward angle measurements with a proton target, and three sets of backward angle measurements with a hydrogen and deuterium target. The measurements are made of the parity-violating asymmetries in elastic electron scattering.;The G0 experiment is a major installation at Jefferson Lab's Hall C with a new dedicated spectrometer. The superconducting magnet is made up of 8 coils with a maximum field of 1.6 T·m. The scintillator detector array (detector solid angle between 0.4--0.9 sr) detects recoiled protons in the forward angle measurement (where thetap = 70° +/- 10° corresponding to scattered electron angles of a few degrees) and to detect scattered electrons in the backward angle measurements. This detector array is made up of a set of 16 pairs of scintillators arranged in 8 sectors around the beam line. Custom electronics handle the high data rate (approximately 1 MHz per detector). The target is a 20 cm long liquid hydrogen cryotarget. Besides the check-out of the new hardware, G 0 has stringent requirements on the performance of the polarized electron beam in order to minimize false asymmetries. Further complicating this fact, in the forward mode, was the requirement that the time structure of the JLab beam had to be changed from 499 MHz to 31 MHz in order to count the recoiled protons in the spectrometer. Data was collected over a 12 day period at the end of the engineering run. These data were analyzed for a Q2 range of 0.1--0.4 (GeV/c) 2 corresponding to measured electroweak asymmetries that ranged from (-4.4 +/- 1.6 +/- 1.6 ppm) to (-8.5 +/- 2.8 +/- 2.5 ppm).
机译:这项工作基于2002年10月至2003年1月在杰斐逊实验室C厅进行的G 0实验的第一轮工程运行。 G0实验将是第一个测量弱中性形状因子:GEZ(Q2),GMZ(Q2)和GAe(Q2)并通过质子提取质子的奇怪形状因子:GEs(Q2)和GMs(Q 2)的实验。 Rosenbluth分离范围为Q 2(0.1--1.0(GeV / c)2)。这将需要四组测量:使用质子靶进行正向角度测量,以及使用氢和氘靶进行三组向后角度测量。这些测量是通过弹性电子散射中违反奇偶校验的不对称性进行的。G0实验是在杰斐逊实验室C厅的主要装置,配备了新的专用光谱仪。超导磁体由8个线圈组成,最大磁场为1.6 T·m。闪烁体探测器阵列(探测器立体角在0.4--0.9 sr之间)在前向角测量中检测反冲质子(其中抽头= 70°+/- 10°对应于几度的散射电子角)并检测其中的散射电子后角测量。该探测器阵列由围绕光束线布置在8个扇区中的一组16对闪烁体组成。定制电子设备可处理高数据速率(每个检测器大约1 MHz)。目标是20厘米长的液态氢低温目标。除了检验新硬件之外,G 0对极化电子束的性能也有严格的要求,以最大程度地减少错误的不对称性。在正向模式下,使这个事实进一步复杂化的是,要求JLab光束的时间结构必须从499 MHz更改为31 MHz,以便计算光谱仪中的反冲质子。在工程运行结束后的12天内收集了数据。分析这些数据的Q2范围为0.1--0.4(GeV / c)2,对应于测量的电弱不对称性,其范围为(-4.4 +/- 1.6 +/- 1.6 ppm)至(-8.5 +/- 2.8 + / -2.5 ppm)。

著录项

  • 作者

    Secrest, Jeffery A.;

  • 作者单位

    The College of William and Mary.;

  • 授予单位 The College of William and Mary.;
  • 学科 Physics Nuclear.;Physics Elementary Particles and High Energy.
  • 学位 Ph.D.
  • 年度 2006
  • 页码 166 p.
  • 总页数 166
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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