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Combining projection superoperators and cumulant expansions in open quantum dynamics with initial correlations and fluctuating Hamiltonians and environments

机译:结合投影超级算子和开放量子动力学中的累积扩展与初始相关性以及波动的哈密顿量和环境

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The evolution of a small system a interacting with a bath b has been described by two different kinds of master equations for its reduced density matrix rho(a) (t): (i) Nakajima-Zwanzig 'memory' equations resulting from the use of projection superoperators; (ii) Time-local equations based on cumulant expansions. It is pointed out that their solution rho(a)(t) may be expressed in the 'hybrid' form (> signifies time-ordering) rho(a)(t) = B(t, tau) + integral(tau)(t) ds B(t, s)C(s, tau), B(t, t') = e(>)(integraltt, ds L(s, t')) where L(s, t') is a cumulant expansion independent of initial correlations, while C(s, tau), defined in terms of projectors, is the initial correlation term appearing in the 'memory' equation. Thus, the convolution represents the effect of initial correlations on rho(a)(t). We analyse the physical meanings of weak coupling approximations to the 'memory' and 'time-local' equations, elucidating why the latter are more accurate in general. We allow time-dependent Hamiltonians and non-stationary bath states. (C) 2003 Elsevier B.V. All rights reserved. [References: 14]
机译:小系统a与浴b相互作用的演化已通过两种不同的降低密度矩阵rho(a)(t)的主方程进行了描述:(i)Nakajima-Zwanzig“记忆”方程是通过使用投影超级运算符; (ii)基于累积量展开的时间局部方程。需要指出的是,它们的解rho(a)(t)可以以``混合''形式表示(>表示时间顺序)rho(a)(t)= B(t,tau)+积分(tau)( t)ds B(t,s)C(s,tau),B(t,t')= e(>)(积分,ds L(s,t'))其中L(s,t')为与初始相关性无关的累积扩展,而根据投影仪定义的C(s,tau)是出现在“内存”方程式中的初始相关性项。因此,卷积表示初始相关对rho(a)(t)的影响。我们分析了“记忆”和“时间局部”方程的弱耦合近似的物理含义,阐明了为什么后者通常更准确。我们允许时间依赖的哈密顿量和非平稳浴状态。 (C)2003 Elsevier B.V.保留所有权利。 [参考:14]

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