diff --git a/src/num_results.tex b/src/num_results.tex
index a47ef6d..e239370 100644
--- a/src/num_results.tex
+++ b/src/num_results.tex
@@ -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 \(h_{i}\)