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some note about the tame regime
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@ -1422,7 +1422,11 @@ system energy change due to the both is of similar magnitude however.
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A periodic steady state is reached after roughly two cycles. In this
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steady state, the system and interaction related quantities are
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constant in the stroboscopic view (the dots in \cref{fig:ottoenergy}),
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while the total energy and the bath energies depend linearly on time.
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while the total energy and the bath energies depend linearly on
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time. We do not see no oscillations in the bath energy which would
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indicate the more complicated energy transfer behaviour we found in
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\cref{sec:one_bath_cutoff}, signifying that we are working in a rather
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``tame'' regime as intended.
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The Gibbs like inequality \cref{eq:secondlaw_cyclic} derived in
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\cref{sec:operational_thermo} can also be verified in this case.
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