Eigenoperator approach to Schrieffer-Wolff perturbation theory and dispersive interactions

Gabriel T. Landi
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Abstract

Modern quantum physics is very modular: we first understand basic building blocks (``XXZ Hamiltonian'' ``Jaynes-Cummings'' etc.) and then combine them to explore novel effects. A typical example is placing known systems inside an optical cavity. The Schrieffer-Wolff perturbation method is particularly suited for dealing with these problems, since it casts the perturbation expansion in terms of operator corrections to a Hamiltonian, which is more intuitive than energy level corrections, as in traditional time-independent perturbation theory. However, the method lacks a systematic approach.% and has largely remained a niche topic. In these notes we discuss how \emph{eigenoperator decompositions}, a concept largely used in open quantum systems, can be employed to construct an intuitive and systematic formulation of Schrieffer-Wolff perturbation theory. To illustrate this we revisit various papers in the literature, old and new, and show how they can instead be solved using eigenoperators. Particular emphasis is given to perturbations that couple two systems with very different transition frequencies (highly off-resonance), leading to the so-called dispersive interactions.
施里弗-沃尔夫扰动理论和分散相互作用的特征算子方法
现代量子物理学是非常模块化的:我们首先了解基本构件("XXZ 哈密顿"、"杰尼斯-康明斯 "等),然后将它们结合起来探索新的效应。一个典型的例子是将已知系统置于光腔内。施里弗-沃尔夫微扰方法特别适合于处理这些问题,因为它把微扰展开的算子修正投射到哈密顿中,这比传统的时间无关微扰理论中的能级修正更直观。然而,这种方法缺乏系统性,在很大程度上仍然是一个小众课题。在这些注释中,我们讨论了如何利用主要用于开放量子系统的 "本征运算分解"(emph{eigenoperatordecompositions})概念来构建施里弗-沃尔夫微扰理论的直观而系统的表述。为了说明这一点,我们重温了新旧文献中的各种论文,并展示了如何利用特征运算符来解决这些问题。我们特别强调了将两个过渡频率截然不同(高度非共振)的系统耦合在一起的扰动,这导致了所谓的色散相互作用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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