From aa3a9b340fafc65c9cee72c1d8c10f5d6f179d77 Mon Sep 17 00:00:00 2001 From: Jaron Kent-Dobias Date: Tue, 15 May 2018 13:42:47 -0400 Subject: added reference to ising.js --- monte-carlo.tex | 5 ++++- 1 file changed, 4 insertions(+), 1 deletion(-) (limited to 'monte-carlo.tex') diff --git a/monte-carlo.tex b/monte-carlo.tex index a305aa8..222d6ed 100644 --- a/monte-carlo.tex +++ b/monte-carlo.tex @@ -395,7 +395,10 @@ Since the symmetry group and the spins are described by the same elements, performing the algorithm on the Ising model in a field is fully described by just using the `ghost spin' representation. This algorithm or algorithms based on the same decomposition of the Hamiltonian have been applied -by several researchers \cite{alexandrowicz_swendsen-wang_1989, wang_clusters_1989, ray_metastability_1990}. +by several researchers \cite{alexandrowicz_swendsen-wang_1989, +wang_clusters_1989, ray_metastability_1990}. The algorithm has been +implemented by one of the authors in an existing interactive Ising +simulator at \texttt{https://mattbierbaum.github.io/ising.js} \cite{bierbaum_ising.js_nodate}. \emph{The $\mathrm O(n)$ model.} In the $\mathrm O(n)$ model spins are described by vectors on the $(n-1)$-sphere $S^{n-1}$. Its symmetry group is $O(n)$, $n\times n$ orthogonal -- cgit v1.2.3-54-g00ecf