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smooth over analytical solution (thx Kimmo)
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@ -6,8 +6,8 @@ The results of \cref{chap:flow} are promising from a numerical
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perspective but remain to be verified. Previous
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work~\cite{Hartmann2017Dec,Hartmann2021Aug,RichardDiss} has made it
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clear that the reduced system dynamics can be efficiently treated by
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the method, but it is an open question whether bath related quantities
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can be calculated to a similar degree of accuracy.
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the NMQSD/HOPS, but it is an open question whether bath related
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quantities can be calculated to a similar degree of accuracy.
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The best possible verification is the comparison with a soluble model,
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ideally treated with a method completely different from the NMQSD. In
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@ -79,8 +79,8 @@ Then
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\end{equation}
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Because we are only interested in solutions for \(t\geq 0\) and the
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shape of the convolution in \cref{eq:eqmotprop} the solution may be
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found by virtue of the Laplace transform.
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appearance of the convolution in \cref{eq:eqmotprop} the solution may
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be found by virtue of the Laplace transform.
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Setting
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\begin{equation}
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@ -360,7 +360,9 @@ now consider a model with two baths.
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The considerations of~\cref{sec:oneosc} can be straight forwardly
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generalized to the case of two coupled oscillators coupled in turn to
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a bath each. This construction is chosen so that the previous results
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can be reused and the coupling to the baths is not trivial.
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can be reused and the coupling to the baths is not trivial. It is
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therefore the simplest generalization of QBM for the relevant
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applications.
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We will not give explicit formulas for the results in terms of sums of
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exponentials, as they are quite extensive and easily obtained via the
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@ -448,7 +450,7 @@ now with a more complicated matrix
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\end{equation}
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which we have to invert.
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This can be done easily\footnote{We have use a computer algebra
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This can be done easily\footnote{We have used a computer algebra
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system. There is probably a pattern to the inverse matrix, so that
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the solution for \(N>2\) oscillators may be found.} and yields
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\begin{equation}
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