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authorJaron Kent-Dobias <jaron@kent-dobias.com>2018-10-22 12:03:19 -0400
committerJaron Kent-Dobias <jaron@kent-dobias.com>2018-10-22 12:03:19 -0400
commit2128a09515fd0b1cb6554eb589377dce5cd4a12c (patch)
tree536ae322ebb6fa54a3b059725a86112fa901a07c
parent887b3ed009138d8fbcd81db335b2991626474d64 (diff)
parentc910b4d9c89426996d7d4e9a3c3bcc8134a94fb4 (diff)
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Merge branch 'master' of git:pub_wolff-field
-rw-r--r--ising_standalone.cpp6
-rw-r--r--monte-carlo.tex10
2 files changed, 5 insertions, 11 deletions
diff --git a/ising_standalone.cpp b/ising_standalone.cpp
index 14c39e7..40572fd 100644
--- a/ising_standalone.cpp
+++ b/ising_standalone.cpp
@@ -32,14 +32,8 @@ class measure_clusters : public measurement<ising_t, ising_t> {
void pre_cluster(N_t, N_t, const system<ising_t, ising_t>&, v_t, const ising_t&) { C = 0; }
- void plain_bond_visited(const system<ising_t, ising_t>&, v_t, const ising_t&, v_t, double) {}
-
- void ghost_bond_visited(const system<ising_t, ising_t>&, v_t, const ising_t&, const ising_t&, double) {}
-
void plain_site_transformed(const system<ising_t, ising_t>&, v_t, const ising_t&) { C++; }
- void ghost_site_transformed(const system<ising_t, ising_t>&, const ising_t&) {}
-
void post_cluster(N_t, N_t, const system<ising_t, ising_t>&) { Ctotal += C; }
};
diff --git a/monte-carlo.tex b/monte-carlo.tex
index f5ff8e7..a0a26fc 100644
--- a/monte-carlo.tex
+++ b/monte-carlo.tex
@@ -187,7 +187,7 @@ redner_graphical_1998}.
integer $k$ and $\theta(s)$ giving the angle of $s$ to some axis applied
to the $\mathrm O(2)$ model \cite{jose_renormalization_1977}. All models
listed here have example implementations in the provided \CXX\ library
- \cite{kent-dobias_2018_wolff}.
+ \cite{kent-dobias_wolff_2018}.
}
\label{table:models}
\end{table*}
@@ -457,7 +457,7 @@ authors in an existing interactive Ising simulator at
\url{https://mattbierbaum.github.io/ising.js}
\cite{bierbaum_ising.js_2016}.
-\subsection{The XY and other $\mathrm O(n)$ models}
+\subsection{The $\mathrm O(n)$ models}
\label{sec:examples:on}
In the $\mathrm O(n)$ model spins are described by vectors on the
@@ -618,9 +618,9 @@ of $hL^{\beta\delta/\nu}$.
model-dependent. Colored lines and points depict values as measured by the
extended algorithm. Solid black lines show a plot proportional to
$h^{-z\nu/\beta\delta}$ for each model. The dynamic exponents $z$ are
- roughly measured as \twodee Ising: 0.23(2), \threedee Ising: 0.28(2),
- \twodee 3-State Potts: 0.55(1), \twodee 4-State Potts: 0.94(5),
- \threedee O(2): 0.17(2), \threedee O(3): 0.13(2). $\mathrm O(n)$ models
+ roughly measured as \twodee Ising: 0.23(5), \threedee Ising: 0.28(5),
+ \twodee 3-State Potts: 0.55(5), \twodee 4-State Potts: 0.94(5),
+ \threedee O(2): 0.17(5), \threedee O(3): 0.13(5). $\mathrm O(n)$ models
use the distribution of transformations described in Section
\ref{sec:examples:on}. The curves stop collapsing at high fields when the
correlation length falls to near the lattice spacing; here non-cluster