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acknowledge valentin by citing his thesis and explain sep phases
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@ -1619,3 +1619,15 @@
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publisher = {American Institute of Physics},
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publisher = {American Institute of Physics},
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doi = {10.1063/1.5022225}
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doi = {10.1063/1.5022225}
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}
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}
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@phdthesis{Link2022Jul,
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author = { Link, Valentin Technische Universität Dresden },
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title = { Stochastic dynamics of open quantum systems with
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applications to nonequilibrium phase transitions },
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keywords = { Hochschulschrift },
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year = 2022,
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institution = {Institut für Theoretische Physik, Technische
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Universität Dresden},
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address = { Dresden },
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url = { http://slubdd.de/katalog?TN_libero_mab216914069 }
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}
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@ -132,10 +132,12 @@ Laplace transformation by expanding the BCF in terms of functions that
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have a simple Laplace transform. As we also use an exponential
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have a simple Laplace transform. As we also use an exponential
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expansion in HOPS and are only interested in finite times, we may
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expansion in HOPS and are only interested in finite times, we may
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choose\footnote{This ansatz was found in private communication with
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choose\footnote{This ansatz was found in private communication with
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Valentin Link \orcidlink{0000-0002-1520-7931}.}
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Valentin Link \cite{Link2022Jul}.}
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\(α_0(t)=\sum_{n=1}^N G_n \eu^{-W_n t - \i \varphi_n}\) with
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\(α_0(t)=\sum_{n=1}^N G_n \eu^{-W_n t - \i \varphi_n}\) with
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\(W_n=\gamma_n + \i\delta_n\) and
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\(W_n=\gamma_n + \i\delta_n\) and
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\(G_n, \varphi_n, \gamma_n,\delta_n\in\RR\) for \(t\geq 0\).
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\(G_n, \varphi_n, \gamma_n,\delta_n\in\RR\) for \(t\geq 0\). We
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separate the phases of the complex numbers involved, as they will
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appear separated from the real parts due to the Laplace transform
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This leads to a mathematically simple expression for the Laplace
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This leads to a mathematically simple expression for the Laplace
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transform
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transform
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