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Stratified quantization approach to dissipative quantum systems: Derivation of the Hamiltonian and kinetic equations for reduced density matrices

机译:耗散量子系统的分层量化方法:降低密度矩阵的哈密顿方程和动力学方程的推导

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A technique for describing dissipative quantum systems that utilizes a fundamental Hamiltonian, which is composed of intrinsic operators of the system, is presented. The specific system considered is a capacitor (or free particle) that is coupled to a resistor (or dissipative medium). The microscopic mechanisms that lead to dissipation are represented by the standard Hamiltonian. Now dissipation is really a collective phenomenon of entities that comprise a macroscopic or mesoscopic object. Hence operators that describe the collective features of the dissipative medium are utilized to construct the Hamiltonian that represents the coupled resistor and capacitor. Quantization of the spatial gauge function is introduced. The magnetic energy part of the coupled Hamiltonian is written in terms of that quantized gauge function and the current density of the dissipative medium. A detailed derivation of the kinetic equation that represents the capacitor or free particle is presented. The partial spectral densities and functions related to spectral densities, which enter the kinetic equations as coefficients of commutators, are evaluated. Explicit expressions for the nonMarkoffian contribution in terms of products of spectral densities and related functions are given. The influence of all two-time correlation functions are considered. Also stated is a remainder term that is a product of partial spectral densities and which is due to higher order terms in the correlation density matrix. The Markoffian part of the kinetic equation is compared with the Master equation that is obtained using the standard generator in the axiomatic approach. A detailed derivation of the Master equation that represents the dissipative medium is also presented. The dynamical equation for the resistor depends on the spatial wavevector, and the influence of the free particle on the diagonal elements (in wavevector space) is stated. (c) 2006 Elsevier Inc. All rights reserved.
机译:提出了一种描述耗散量子系统的技术,该技术利用了基本的哈密顿量,该哈密顿量由系统的内在算符组成。所考虑的特定系统是耦合到电阻器(或耗散介质)的电容器(或自由粒子)。导致耗散的微观机制由标准哈密顿量表示。现在,耗散实际上是构成宏观或介观对象的实体的集体现象。因此,描述耗散介质集体特征的算子被用来构造代表耦合的电阻器和电容器的哈密顿量。介绍了空间量表功能的量化。耦合哈密顿量的磁能部分用该量化的量规函数和耗散介质的电流密度来表示。给出了代表电容器或自由粒子的动力学方程的详细推导。评估了部分光谱密度和与光谱密度有关的函数,这些函数作为交换子的系数进入动力学方程。根据频谱密度和相关函数的乘积,给出了非马尔科夫贡献的显式表达式。考虑所有两次相关函数的影响。还说明了剩余项,它是部分频谱密度的乘积,并且是由于相关密度矩阵中的高阶项。将动力学方程式的Markoffian部分与使用公理化方法中的标准生成器获得的Master方程进行比较。还介绍了代表耗散介质的Master方程的详细推导。电阻器的动力学方程取决于空间波矢,并阐明了自由粒子对对角元素(在波矢空间中)的影响。 (c)2006 Elsevier Inc.保留所有权利。

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