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authorJaron Kent-Dobias <jaron@kent-dobias.com>2023-06-16 22:34:16 +0200
committerJaron Kent-Dobias <jaron@kent-dobias.com>2023-06-16 22:34:16 +0200
commit71fd66d16d6a50e61182e48d93bb29624ebf57c0 (patch)
tree028c71e30a862a4acb813c144cafeeb9faa9a32a
parentb5b2b7eef46084fe02594f15861a17a20a1a1289 (diff)
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Fixed typo.
-rw-r--r--when_annealed.tex2
1 files changed, 1 insertions, 1 deletions
diff --git a/when_annealed.tex b/when_annealed.tex
index 537381a..2dd2206 100644
--- a/when_annealed.tex
+++ b/when_annealed.tex
@@ -192,7 +192,7 @@ among ground-state minima \cite{Kent-Dobias_2023_How}.
In these models, trivial correlations between stationary points correspond with
zero overlap: almost all stationary points are orthogonal to each other. This
corresponds with \emph{replica symmetric} (\textsc{rs}) order. The emergence of
-nontrivial correlations, and the invalidity of the anneal approximation, occurs
+nontrivial correlations, and the invalidity of the annealed approximation, occurs
when some non-vanishing fraction of stationary point pairs have a nonzero
overlap. This corresponds to some kind of \emph{replica symmetry breaking}
(\textsc{rsb}). Here we restrict ourselves to a {\oldstylenums1}\textsc{rsb}