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authorJaron Kent-Dobias <jaron@kent-dobias.com>2018-10-02 20:21:15 -0400
committerJaron Kent-Dobias <jaron@kent-dobias.com>2018-10-02 20:21:15 -0400
commit7a850654493f2f5ff42c0e2b611ba018545ac72b (patch)
tree28bab2818667a8cc3edf6755258d1da9eea4af29
parent989e064fbb32c7fd222603136bb7e01d5de66566 (diff)
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one However to Fortunately
-rw-r--r--monte-carlo.tex2
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diff --git a/monte-carlo.tex b/monte-carlo.tex
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--- a/monte-carlo.tex
+++ b/monte-carlo.tex
@@ -257,7 +257,7 @@ caracciolo_wolff-type_1993}.
This algorithm relies on the fact that the coupling $\J$ depends only on
relative orientation of the spins---global reorientations do not affect the
-Hamiltonian. The external field $B$ breaks this symmetry. However, it can be
+Hamiltonian. The external field $B$ breaks this symmetry. Fortunately it can be
restored. Define a new graph $\tilde G=(\tilde V,\tilde E)$, where $\tilde
V=\{0,1,\ldots,N\}$ adds the new `ghost' site $0$ which is connected by
\[