Redfield equation bath correlation functions

Here the W are operators of the subsystem and the superscript dagger denote the Hermitian conjugate. The Redfield equation can be written in this form only when an additional symmetrization of the bath correlation functions is performed [48]. Note that this alternative equation also expresses the dissipative evolution of the density matrix in terms of N x N... 

To evaluate the correlation functions in Eqs. (12) and (13), it is usual to complete the separation of the system and bath by decomposing the system-bath coupling into a sum of products of pure system and bath operators. This allows the correlation functions of the system-bath coupling to be replaced, without loss of generality, by correlation functions of bath operators alone, evolving under the uncoupled bath Hamiltonian. Moreover, as we have previously pointed out [39,40], this decomposition of the system-bath coupling make it possible to write the Redfield equation in a highly compact form, without explicit reference to the Redfield tensor at all. 

There are three important issues to consider in the numerical solution of the Redfield equation. The first is the evaluation of the Redfield tensor matrix elements I ,To obtain these matrix elements, it is necessary to have a representation of the system-bath coupling operator and of the bath Hamiltonian. Two fundamental types of models are used. First, the system-bath coupling can be described using stochastic fluctuation operators, without reference to a microscopic model. In this case, the correlation functions appearing in the formulas for parame-... 

An important feature of the reduced-density-matrix approach is that it allows the bath to be treated at different levels of approximation. In the Redfield equation, the bath enters only through the correlation functions of the coupled bath variables in Eq. (18). This means that a substantial part of the complexity of a realistic condensed-phase environment is... 

To use this final result in the Redfield equation, all of the autocorrelation and crosscorrelation functions of these five bath operators will be required to define the 0 matrices in Eq. (18) these can all be obtained by standard techniques [32]. For reference, the required correlation functions are summarized in the Appendix. Note that the operators F+ and F are not Hermitian, so that the general form of the Redfield equation [Eq. (20)] must be used. 

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