From aa3a9b340fafc65c9cee72c1d8c10f5d6f179d77 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
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

