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Measurement of the weak mixing angle in Moller scattering.

机译:测量穆勒散射中的弱混合角。

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摘要

The weak mixing parameter, sin2q w , is one of the fundamental parameters of the Standard Model. Its tree-level value has been measured with high precision at energies near the Z0 pole; however, due to radiative corrections at the one-loop level, the value of sin2q w is expected to change with the interaction energy. As a result, a measurement of sin2q w at low energy (Q2 ≪ mZ, where Q2 is the momentum transfer and mZ is the Z boson mass), provides a test of the Standard Model at the one-loop level, and a probe for new physics beyond the Standard Model.; One way of obtaining sin2q w at low energy is from measuring the left-right, parity-violating asymmetry in electron-electron (Moller) scattering: APV = sR-sLs R+sL , where sigmaR and sigma L are the cross sections for right- and left-handed incident electrons, respectively. The parity violating asymmetry is proportional to the pseudo-scalar weak neutral current coupling in Moller scattering, gee. At tree level gee = (¼ - sin2q w ). A precision measurement of the parity-violating asymmetry in Moller scattering was performed by Experiment E158 at the Stanford Linear Accelerator Center (SLAC). During the experiment, ∼50 GeV longitudinally polarized electrons scattered off unpolarized atomic electrons in a liquid hydrogen target, corresponding to an average momentum transfer Q 2 ∼ 0.03 (GeV/c)2. The tree-level prediction for APV at such energy is ≃300 ppb. However one-loop radiative corrections reduce its value by ∼40%.; This document reports the E158 results from the 2002 data collection period. The parity-violating asymmetry was found to be APV = -160 +/- 21 (stat.) +/- 17 (syst.) ppb, which represents the first observation of a parity-violating asymmetry in Moller scattering. This value corresponds to a weak mixing angle at Q 2 = 0.026 (GeV/c)2 of sin2q wMS = 0.2379 +/- 0.0016 (stat.) +/- 0.0013 (syst.), which is -0.3 standard deviations away from the Standard Model prediction: sin2q predictedw MS = 0.2385 +/- 0.0006 (theory). The E158 measurement of sin2q w at a precision of delta( sin2q w ) = 0.0020 provides new physics sensitivity at the TeV scale.
机译:弱混合参数sin2q w是标准模型的基本参数之一。已经在Z0极附近的能量下以高精度测量了其树级值;然而,由于在单回路水平进行辐射校正,sin2q w的值预计会随着相互作用能而变化。结果,在低能量(Q2≪ mZ,其中Q2是动量传递,mZ是Z玻色子质量)下的sin2q w的测量提供了单环水平的标准模型测试和探针用于标准模型之外的新物理。在低能量下获得sin2q w的一种方法是通过测量电子-电子(Moller)散射中的左右,违反奇偶性的不对称性:APV = sR-sLs R + sL,其中sigmaR和sigma L是右边的横截面-和左手入射电子。违反奇偶校验的不对称性与Moller散射gee中的准标量弱中性电流耦合成比例。在树级别,gee =(¼-sin2q w)。斯坦福线性加速器中心(SLAC)的实验E158对Moller散射中违反奇偶校验的不对称性进行了精确测量。在实验过程中,〜50 GeV的纵向极化电子从液态氢靶中的非极化原子电子中散射出来,相当于平均动量传递Q 2〜0.03(GeV / c)2。在这样的能量下,APV的树级预测为≃ 300 ppb。但是,单回路辐射校正将其值降低了约40%。本文档报告了2002年数据收集期间的E158结果。发现违反奇偶性的不对称性是APV = -160 +/- 21(统计)+/- 17(系统)ppb,这是在穆勒散射中首次发现违反奇偶性的不对称性。该值对应于sin2q的Q 2 = 0.026(GeV / c)2时的弱混合角wMS = 0.2379 +/- 0.0016(stat。)+/- 0.0013(syst。),与-0.3的标准偏差为-0.3。标准模型预测:sin2q预测w MS = 0.2385 +/- 0.0006(理论值)。 E158测量sin2q w的精度为delta(sin2q w)= 0.0020,可在TeV尺度上提供新的物理灵敏度。

著录项

  • 作者

    Bega, Klejda.;

  • 作者单位

    California Institute of Technology.;

  • 授予单位 California Institute of Technology.;
  • 学科 Physics Elementary Particles and High Energy.
  • 学位 Ph.D.
  • 年度 2004
  • 页码 112 p.
  • 总页数 112
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 高能物理学;
  • 关键词

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