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Measuring the electron electric dipole moment using laser-cooled cesium atoms in optical lattices.

机译:在光学晶格中使用激光冷却的铯原子测量电子偶极矩。

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摘要

Discrete symmetries have played a vital role in the development of the standard model of particle physics. Electric dipole moments (EDM's) of elementary particles are sensitive probes of discrete symmetry violations. The standard model predicts a permanent electron electric dipole moment (eEDM) that is 10--37 ∼10--38 e · cm. Most proposed standard model extensions, like supersymmetry, predict a larger eEDM that is comparable to or slightly smaller than the current experimental limit, |de| ≤ 1.05 x 10 -27 e · cm. Observation of a permanent eEDM in the foreseeable future would imply new CP violating effects not captured by the standard model. This dissertation is a project report of the Penn State eEDM search using laser-cooled Cesium atoms in optical lattices. In particular, I will describe experimental progress in apparatus development, quantum state preparation and state-selective fluorescence detection, and magnetometry using Larmor precession of spin-polarized atoms. I will also describe theoretical studies of low frequency spectroscopy that will be used in the eEDM measurements. In our experiment, Cesium atoms are guided into a measurement chamber, where they are laser-cooled and trapped in a pair of far-detuned, high quality linearly polarized, parallel one-dimensional optical lattices. The lattice beams thread three specially coated fused silica electric field plates. The measurement chamber is passively shielded by a four layer mu-metal magnetic shield, inside of which eight magnetic field coils actively control the bias and gradient magnetic fields, based on sensitive atomic magnetometry measurements. A series of high fidelity microwave adiabatic fast passage pulses and specially engineered low frequency magnetic pulses transfer the atoms into a superposition state that is sensitive to the eEDM signal. Combining unprecedented precision made possible by cold atoms with engineering, our experiment has a projected precision that is 400-fold improvement of the current measured limit.
机译:离散对称性在粒子物理学标准模型的开发中起着至关重要的作用。基本粒子的电偶极矩(EDM)是离散对称违规的敏感探针。标准模型预测的永久电子偶极矩(eEDM)为10--37〜10--38 e·cm。大多数提议的标准模型扩展(如超对称性)都可以预测一个更大的eEDM,该eEDM与当前的实验极限| de |相当或略小。 ≤1.05 x 10 -27 e·cm。在可预见的将来观察到永久性eEDM将意味着标准模型未捕获到新的CP违规效应。本论文是宾夕法尼亚州eEDM搜索的一个项目报告,该eEDM使用光学晶格中的激光冷却铯原子进行搜索。特别是,我将描述设备开发,量子态制备和状态选择性荧光检测以及使用自旋极化原子的拉莫尔进动的磁力计的实验进展。我还将描述将用于eEDM测量的低频光谱学的理论研究。在我们的实验中,铯原子被引导到测量室中,在那里它们被激光冷却并被捕获在一对失谐的,高质量的线性偏振,平行的一维光学晶格中。晶格束穿过三个特殊涂层的熔融石英电场板。测量室由四层mu-metal磁屏蔽罩被动屏蔽,在该屏蔽罩的内部有八个磁场线圈根据灵敏的原子磁力测量法主动控制偏置磁场和梯度磁场。一系列高保真微波绝热快速通过脉冲和经过特殊设计的低频磁脉冲将原子转移到对eEDM信号敏感的叠加状态。将冷原子带来的空前精度与工程技术相结合,我们的实验的预计精度是当前测量极限的400倍。

著录项

  • 作者

    Zhu, Kunyan.;

  • 作者单位

    The Pennsylvania State University.;

  • 授予单位 The Pennsylvania State University.;
  • 学科 Physics Low Temperature.
  • 学位 Ph.D.
  • 年度 2013
  • 页码 221 p.
  • 总页数 221
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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