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fix typo

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Valentin Boettcher 2022-08-31 16:26:28 +02:00
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12
src/num_results.tex
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@ -1367,12 +1367,12 @@ compressed (cold) or expanded (hot) state. Their magnitudes have been
chosen so that their values at these points are the same as can be
seen in \cref{fig:ottomod}.
We initialize the system in the \(H_{\sys}\ket{0}=0\) state.
For the demonstration we chose \(T_{c}=1\) and \(T_{h}=20\) so that
both temperatures are finite but not so high that a reasonable number
of samples is required for convergence. The interaction strength has
been chosen to be relatively weak for the same reason and to be closer
to the known weak coupling realm.
We initialize the system in the \(H_{\sys}\ket{0}=0\) state. For the
demonstration we chose \(T_{c}=1\) and \(T_{h}=20\) so that both
temperatures are finite but not so high that an unreasonable number of
samples is required for convergence. The interaction strength has been
chosen to be relatively weak for the same reason and to be closer to
the known weak coupling realm.
In comparison to the system time scale, the modulation cycle is rather
slow. On the other hand, the time scales on which \(f\) and \(h_{i}\)