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@ -1129,7 +1129,7 @@ bath correlation function.
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simulations with small \(ω_{c}\) the positive parts of the interaction
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energy are especially large.
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For very weak coupling \(\ev{H_{\inter}}\approx .01\)
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For very weak coupling \(\ev{H_{\inter}}\approx 0.01\)
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\cref{fig:omega_couplings_weak} shows that this optimization procedure
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yields the normalization of \cref{eq:normohmic}. This is plausible,
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because for weaker coupling the initial slip phase upon which
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