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Quantum electrodynamics of a driven three-level atom near the edge of a photonic band gap.

机译:被驱动的三能级原子在光子带隙边缘附近的量子电动力学。

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摘要

In the first part of this thesis, the coherent control of spontaneous emission for a three level atom located within a photonic band gap (PBG) material is demonstrated. Spontaneous emission from the three level atom can be totally suppressed or strongly enhanced depending on the relative phase between the steady-state control laser coupling the two upper levels and the pump laser pulse used to create an excited state of the atom in the form of a coherent superposition of the two upper levels. Unlike the free space case, the steady-state inversion of the atomic system is strongly dependent on the externally prescribed initial conditions. This non-zero steady state population is robust to decoherence effects provided that the Rabi frequency of the control laser field exceeds the rate of dephasing interactions. As a result, such a system may be relevant for a single-atom, phase sensitive, optical memory device on the atomic scale. Provided that coherence can be maintained between the two upper atomic levels, the model system can also act as a qubit to encode information for quantum computation.; In the second part of this thesis, the resonance Raman scattering of light from a three-level atom in the Λ configuration embedded in a photonic band gap material is studied as a direct experimental probe for the photon-atom bound state discussed in the first part. The one particle spectrum of the system is demonstrated to consist of either a continuous part with energy lying outside the gap or a single discrete mode with energy lying inside the gap. The discrete mode, which occurs when both of the allowed atomic transitions lie inside the gap, can be treated as a photon-atom bound state in which the radiation is localized in the vicinity of the atom. In the case of the continuous spectrum, the Rayleigh and Stokes lines are shifted as well as narrowed (or broadened) as the corresponding transition frequencies are shifted relative to the upper band edge, providing a distinctive experimental signature of atom-photon interactions near a photonic band edge.
机译:在本文的第一部分,对位于光子带隙(PBG)材料中的三能级原子的自发发射进行了相干控制。根据耦合到两个较高能级的稳态控制激光器和用于产生原子激发态的泵浦激光脉冲之间的相对相位,可以完全抑制或强烈增强三能级原子的自发发射。两个较高层次的连贯叠加。与自由空间情况不同,原子系统的稳态反转在很大程度上取决于外部规定的初始条件。如果控制激光场的拉比频率超过移相作用的速率,则该非零稳态种群对于退相干效应具有鲁棒性。结果,这样的系统在原子尺度上可能与单原子,相敏感的光学存储设备有关。假设可以在两个较高原子级之间保持相干性,则模型系统还可以充当量子位来编码信息以进行量子计算。在本文的第二部分中,研究了嵌入在光子带隙材料中的Λ构型的三能级原子发出的共振拉曼散射,作为在第一部分中讨论的光子-原子束缚态的直接实验探针。 。系统的一个粒子光谱被证明由能量位于间隙外部的连续部分或能量位于间隙内部的单个离散模式组成。当两个允许的原子跃迁都位于间隙内时发生的离散模式可以视为光子-原子束缚状态,其中辐射位于原子附近。在连续光谱的情况下,随着相应的跃迁频率相对于上带边缘的偏移,瑞利和斯托克斯线也发生偏移和变窄(或变宽),从而在光子附近提供了原子-光子相互作用的独特实验特征乐队边缘。

著录项

  • 作者单位

    University of Toronto (Canada).;

  • 授予单位 University of Toronto (Canada).;
  • 学科 Physics Optics.
  • 学位 Ph.D.
  • 年度 2001
  • 页码 168 p.
  • 总页数 168
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 光学;
  • 关键词

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