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@@ -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