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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2018-09-25 16:43:58 -0400 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2018-09-25 16:43:58 -0400 |
commit | e6f638a736629a97f210b856fcded51a7ef09813 (patch) | |
tree | 1337c77034066f0bc11cca31595ab7fe043ce5ac | |
parent | 71d7e69a293d0d037a6a7b10308ba8d4a072fcf5 (diff) | |
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clarification to discussion of former work on SOS algorithms
-rw-r--r-- | monte-carlo.tex | 3 |
1 files changed, 2 insertions, 1 deletions
diff --git a/monte-carlo.tex b/monte-carlo.tex index 57f3859..4b9ba61 100644 --- a/monte-carlo.tex +++ b/monte-carlo.tex @@ -434,8 +434,9 @@ $s_i\cdot j=-i-j$. The elements of order two are reflections $s_i$, whose action on $\Z$ is transitive. The coupling can be any function of the absolute difference $|i-j|$. Because random choice of reflection will almost always result in energy changes so large that the whole system is flipped, it is -better to select random reflections about integers close to the average state +better to select random reflections about integers or half-integers close to the average state of the system. A variant of the algorithm has been applied without a field +whose success relies both on this and on using nonzero $q$ \cite{evertz_stochastic_1991}. \section{Performance} |