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authorJaron Kent-Dobias <jaron@kent-dobias.com>2023-08-23 19:40:59 +0200
committerJaron Kent-Dobias <jaron@kent-dobias.com>2023-08-23 19:40:59 +0200
commit74d620a5c17a32cb90a885adff12d1c75d4ab31c (patch)
tree7c525388f633f55dd867a4263cfda3900bd52fb5
parent0eef1bbb39d6aa9ee0251429659f89783e6bc2e2 (diff)
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Small spot changes.
-rw-r--r--when_annealed.tex6
1 files changed, 3 insertions, 3 deletions
diff --git a/when_annealed.tex b/when_annealed.tex
index 0304218..cbbe4f9 100644
--- a/when_annealed.tex
+++ b/when_annealed.tex
@@ -30,7 +30,7 @@
counts are reliably found by taking the average of the logarithm (the
quenched average), which is more difficult and not often done in practice.
When most stationary points are uncorrelated with each other, quenched and
- anneals averages are equal. Equilibrium heuristics can guarantee when most of
+ annealed averages are equal. Equilibrium heuristics can guarantee when most of
the lowest minima will be uncorrelated. We show that these equilibrium
heuristics cannot be used to draw conclusions about other minima and saddles
by producing examples among Gaussian-correlated functions on the hypersphere
@@ -362,7 +362,7 @@ $e$, $g$, and $h$ are given by
transition, coincides with it in this case. The gray shaded region
highlights the minima, which are stationary points with $\mu\geq\mu_\mathrm
m$. $E_\textrm{min}$ is marked on the plot as the lowest energy at which
- extensive saddles are found.
+ saddles of extensive index are found.
} \label{fig:complexity_35}
\end{figure}
@@ -450,7 +450,7 @@ of saddles $E_\mathrm{min}$. Also, these models have a transition boundary that
smoothly connects $E_{\oldstylenums1\textsc{rsb}}^+$ and
$E_{\oldstylenums1\textsc{rsb}}^-$, so $E_{\oldstylenums1\textsc{rsb}}^-$
corresponds to the lower bound of \textsc{rsb} complexity. For large enough
-$s$, the range passes into minima, which is excepted as these models have
+$s$, the range passes into minima, which is expected as these models have
nontrivial complexity of their ground states. This also seems to correspond
with the decoupling of the \textsc{rsb} solutions connected to
$E_{\oldstylenums1\textsc{rsb}}^+$ and $E_{\oldstylenums1\textsc{rsb}}^-$, with