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Gauge invariance of phenomenological models of the interaction of quantum dissipative systems with electromagnetic fields

机译:量子耗散系统与电磁场相互作用的现象学模型的量规不变性

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We discuss specific features of the electrodynamic characteristics of quantum systems within the framework of models that include a phenomenological description of the relaxation processes. As is shown by W. E. Lamb, Jr., R. R. Schlicher, and M. 0. Scully [Phys. Rev. A 36, 2763 (1987)], the use of phenomenological relaxation operators, which adequately describe the attenuation of eigenvibrations of a quantum system, may lead to incorrect solutions in the presence of external electromagnetic fields determined by the vector potential for different resonance processes. This incorrectness can be eliminated by giving a gauge-invariant form to the relaxation operator. Lamb, Jr., et al. proposed the corresponding gauge-invariant modification for the Weisskopf-Wigner relaxation operator, which is introduced directly into the Schrodinger equation within the framework of the two-level approximation. In the present paper, this problem is studied for the von Neumann equation supplemented by a relaxation operator. First, we show that the solution of the equation for the density matrix with the relaxation operator correctly obtained "from the first principles" has properties that ensure gauge invariance for the observables. Second, we propose a common recipe for transformation of the phenomenological relaxation operator into the correct (gauge-invariant) form in the density-matrix equations for a multilevel system. Also, we discuss the methods of elimination of other inaccuracies (not related to the gauge-invariance problem) which arise if the electrodynamic response of a dissipative quantum system is calculated within the framework of simplified relaxation models (first of all, the model corresponding to constant relaxation rates of coherences in quantum transitions). Examples illustrating the correctness of the results obtained within the framework of the proposed methods in contrast to inaccuracy of the results of the standard calculation techniques are given.
机译:我们在模型的框架内讨论量子系统电动力学特征的特定特征,其中包括弛豫过程的现象学描述。正如W. E. Lamb,Jr.,R。R. Schlicher和M. 0所示。 Rev. A 36,2763(1987)]中,现象学弛豫算子的使用充分描述了量子系统本征振动的衰减,在存在由不同共振的矢量势确定的外部电磁场的情况下,可能导致错误的解流程。通过给松弛算子赋予量规不变的形式,可以消除这种不正确性。小羔羊等。提出了Weisskopf-Wigner弛豫算子的相应规范不变修正,并将其直接引入到两层近似框架内的Schrodinger方程中。在本文中,对由松弛算子补充的冯·诺依曼方程研究了这个问题。首先,我们证明了使用“根据第一原理”正确获得的具有松弛算子的密度矩阵方程的解具有可确保观测值的规范不变的性质。其次,我们提出了将现象学弛豫算子转换为多级系统的密度矩阵方程中正确的(量规不变)形式的通用方法。此外,我们还讨论了消除其他误差的方法(与规范不变性无关),这些误差是在简化弛豫模型(首先是与量子跃迁中相干的恒定弛豫率)。给出了一些示例,这些示例说明了在所提出的方法的框架内获得的结果的正确性,与标准计算技术的结果的准确性相比。

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