From bc04424456379aa753d31fbf63ffd8b9bcb6f7e3 Mon Sep 17 00:00:00 2001 From: Jaron Kent-Dobias Date: Sun, 21 Oct 2018 22:59:02 -0400 Subject: newest version of the ising example --- ising_standalone.cpp | 6 ------ 1 file changed, 6 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 { void pre_cluster(N_t, N_t, const system&, v_t, const ising_t&) { C = 0; } - void plain_bond_visited(const system&, v_t, const ising_t&, v_t, double) {} - - void ghost_bond_visited(const system&, v_t, const ising_t&, const ising_t&, double) {} - void plain_site_transformed(const system&, v_t, const ising_t&) { C++; } - void ghost_site_transformed(const system&, const ising_t&) {} - void post_cluster(N_t, N_t, const system&) { Ctotal += C; } }; -- cgit v1.2.3-54-g00ecf From 3c0d214240facb7e79c8f4953265ca175d928fe3 Mon Sep 17 00:00:00 2001 From: Jaron Kent-Dobias Date: Sun, 21 Oct 2018 23:02:44 -0400 Subject: no strong statements about exponents! --- monte-carlo.tex | 6 +++--- 1 file changed, 3 insertions(+), 3 deletions(-) diff --git a/monte-carlo.tex b/monte-carlo.tex index f5ff8e7..76a4103 100644 --- a/monte-carlo.tex +++ b/monte-carlo.tex @@ -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 -- cgit v1.2.3-54-g00ecf From 16915b8d270d92dab7dba945cd90e16f02bca353 Mon Sep 17 00:00:00 2001 From: Jaron Kent-Dobias Date: Sun, 21 Oct 2018 23:52:06 -0400 Subject: changed section header in examples back to O(n) --- monte-carlo.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/monte-carlo.tex b/monte-carlo.tex index 76a4103..aec3bc5 100644 --- a/monte-carlo.tex +++ b/monte-carlo.tex @@ -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 -- cgit v1.2.3-54-g00ecf From c910b4d9c89426996d7d4e9a3c3bcc8134a94fb4 Mon Sep 17 00:00:00 2001 From: Jaron Kent-Dobias Date: Sun, 21 Oct 2018 23:53:31 -0400 Subject: fixed citation --- monte-carlo.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/monte-carlo.tex b/monte-carlo.tex index aec3bc5..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*} -- cgit v1.2.3-54-g00ecf