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Coherent dynamics in atom-field interactions.

机译:原子-场相互作用中的相干动力学。

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摘要

This dissertation treats quantum open system dynamics, focusing on the coherent evolution of a two-level atom (as the system) interacting with an electromagnetic field (as the bath), for purposes relevant to quantum computing. In order to maintain the quantum correlations that develop between the system and bath throughout the evolution path integral formalisms such as the influence functional and closed time path formalisms are used. Predictions of effects due to the quantum correlations in the composite interacting system are computed.; Conventional treatments using Schrödinger-master equation and Heisenberg-Langevin approaches usually ignore system+bath quantum correlations as a technical simplification. It is argued that although neglect of system+bath correlations is generally a good approximation when the bath has a large continuous set of degrees of freedom, a residual coherence effect remains due to the non-zero bath correlation time. Though small, these effects are becoming more relevant as, with the advent of ultra cold atom sources, atom optics experiments are reaching levels at which such residual effects are becoming measurable.; Three specific problems are investigated in this thesis: First is a self-dressing rederivation of the Casimir-Polder retardation force. The well known stationary atom result is reproduced and a result for a slowly moving atom is obtained which is up to twice the stationary atom correction. Second is the entangled evolution of a qubit with an initially thermal low temperature bath. The diagonal matrix elements are found to thermalize and the off-diagonal elements to decohere as expected, however they do so non-exponentially due to the quantum correlations that develop between the qubit and bath. Third is a calculation of qubit dynamics in the presence of quantized atomic motion as well as zero point fluctuations of the electromagnetic field. The decoherence rate of the qubit is found to increase slightly in that case due to the additional degree of freedom.
机译:本文研究量子开放系统动力学,着眼于与量子计算相关的两级原子(作为系统)与电磁场(作为浴)相互作用的相干演化。为了维持在整个演化路径中系统与熔池之间发展的量子相关性,使用了积分形式主义,例如影响功能和封闭时间路径形式主义。计算了由于复合相互作用系统中的量子相关性而产生的效应预测。使用Schrödinger-master方程和Heisenberg-Langevin方法的常规处理通常会忽略系统+浴量子相关性,这是技术上的简化。有人认为,尽管当浴池具有较大的连续自由度集时,通常忽略系统+浴池相关性是一个很好的近似值,但由于浴池相关性时间不为零,因此残留的相干效应仍然存在。尽管影响很小,但随着超冷原子源的出现,这些效应变得越来越相关,因为原子光学实验已达到可以测量这种残余效应的水平。本文研究了三个具体的问题:首先是卡西米尔-波德减速力的自装扮化。再现了众所周知的固定原子结果,并获得了一个慢速移动原子的结果,该结果是固定原子校正的两倍。其次是量子比特与最初低温热浴的纠缠演化。发现对角矩阵元素会发生热化,而对角线元素会发生热分解,但是,由于量子位和镀液之间的量子相关性,它们对角非指数化。第三是在存在量化原子运动以及电磁场的零点波动的情况下计算量子位动力学。在那种情况下,由于附加的自由度,发现量子比特的去相干率略有增加。

著录项

  • 作者

    Shresta, Sanjiv.;

  • 作者单位

    University of Maryland College Park.;

  • 授予单位 University of Maryland College Park.;
  • 学科 Physics Atomic.
  • 学位 Ph.D.
  • 年度 2003
  • 页码 p.4418
  • 总页数 194
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 分子物理学、原子物理学;
  • 关键词

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