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Light pulse Talbot-Lau interferometry with magnetically guided atoms.

机译:具有磁导原子的光脉冲Talbot-Lau干涉仪。

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摘要

This thesis discusses the development of an interferometry experiment with magnetically guided atoms using optical standing wave pulses. Ground-state rubidium atoms are confined in a two-dimensional magnetic quadruple field as a guiding potential. An optical standing wave field is pulsed to transfer photon recoil momentum to atoms. We use several Talbot-Lau type interferometry schemes to study the coherence properties of guided atoms, in particular, we identify an interferometry regime where matter-wave dephasing due to the confined motion are suppressed, allowing long coherence time and high precision measurements. This thesis summarizes the design, construction and operation of the experimental apparatus. We discuss the realization of a guided atom accelerometer, precise recoil frequency measurements with guided atoms, an area-enclosing interferometer based on a moving guide for rotation sensing, and a new interferometry configuration to realize a spatial-displacement echo with up to 1s coherence time and with frozen transverse-confinement induced dephasing.; The matter-wave dephasing due to variations of the guiding potential along the nearly-free direction of propagation is identified as the limiting factor on the achievable interferometry precision, which is likely due to the poling inhomogeneities of the ferro-magnetic foils that generate the guiding potential. Two future options using either a precisely-fabricated atom chip or an optical dipole trap are suggested to overcome the difficulty. As the theoretical part of this thesis, a vector theory of the generalized Talbot-Lau type interferometry is discussed using Weyl functions.
机译:本文讨论了利用光学驻波脉冲对磁导原子进行干涉测量实验的发展。基态rub原子被限制在二维磁四重磁场中作为引导电势。脉冲光驻波场将光子反冲动量传递给原子。我们使用几种Talbot-Lau型干涉测量方案来研究被引导原子的相干特性,特别是,我们确定了一种干涉测量方案,在该方案中可以抑制由于受限运动引起的物质波相移,从而实现长相干时间和高精度测量。本文对实验装置的设计,结构和运行进行了总结。我们讨论了制导原子加速度计的实现,用制导原子进行的精确反冲频率测量,基于用于旋转感应的移动导引的包围式干涉仪以及新的干涉仪配置,以实现具有高达1s相干时间的空间位移回波以及冻结的横向约束引起的相移。由于沿几乎自由的传播方向的引导电位的变化而引起的物波移相被确定为可达到的干涉测量精度的限制因素,这很可能是由于产生引导的铁磁箔的极化不均匀性引起的潜在。建议使用精确制造的原子芯片或光学偶极阱的两种未来选择来克服这一困难。作为本文的理论部分,利用Weyl函数讨论了广义Talbot-Lau型干涉测量的矢量理论。

著录项

  • 作者

    Wu, Saijun.;

  • 作者单位

    Harvard University.;

  • 授予单位 Harvard University.;
  • 学科 Physics Atomic.; Physics Optics.
  • 学位 Ph.D.
  • 年度 2007
  • 页码 370 p.
  • 总页数 370
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 分子物理学、原子物理学;光学;
  • 关键词

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