summaryrefslogtreecommitdiff
path: root/statphys27.tex
diff options
context:
space:
mode:
authorJaron Kent-Dobias <jaron@kent-dobias.com>2019-07-06 10:55:07 -0400
committerJaron Kent-Dobias <jaron@kent-dobias.com>2019-07-06 10:55:07 -0400
commit736908493db28e892d19d7b6a63bdef1372dd196 (patch)
tree3fe44dcbb82c0961610ea70f3ee5a9ca13cb6187 /statphys27.tex
parenteee8a108b8592b23778b642d5785a8ba0773e3bb (diff)
downloadstatphys_27-736908493db28e892d19d7b6a63bdef1372dd196.tar.gz
statphys_27-736908493db28e892d19d7b6a63bdef1372dd196.tar.bz2
statphys_27-736908493db28e892d19d7b6a63bdef1372dd196.zip
lots of new figures
Diffstat (limited to 'statphys27.tex')
-rw-r--r--statphys27.tex27
1 files changed, 27 insertions, 0 deletions
diff --git a/statphys27.tex b/statphys27.tex
index 4c2387b..2524aef 100644
--- a/statphys27.tex
+++ b/statphys27.tex
@@ -23,6 +23,33 @@
\begin{frame}
\frametitle{Monte Carlo is too slow}
+
+ \begin{columns}
+ \begin{column}{0.5\textwidth}
+ Critical timescales diverge like $L^z$.
+
+ \vspace{2em}
+
+ For 2D Ising local algorithms have $z\simeq2$--4.
+
+ \vspace{2em}
+
+ Cluster methods have $z\simeq0.3$!
+
+ \vspace{2em}
+
+
+
+ \end{column}
+ \begin{column}{0.5\textwidth}
+ \begin{overprint}
+ \onslide<1>\includegraphics[width=\columnwidth]{figs/ising_hl_0_0}
+ \onslide<2,4>\includegraphics[width=\columnwidth]{figs/ising_hl_0_1}
+ \onslide<5>\includegraphics[width=\columnwidth]{figs/ising_hl_0_2}
+ \onslide<3,6>\includegraphics[width=\columnwidth]{figs/ising_hl_0_3}
+ \end{overprint}
+ \end{column}
+ \end{columns}
\end{frame}
\begin{frame}