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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2019-07-06 10:55:07 -0400 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2019-07-06 10:55:07 -0400 |
commit | 736908493db28e892d19d7b6a63bdef1372dd196 (patch) | |
tree | 3fe44dcbb82c0961610ea70f3ee5a9ca13cb6187 /statphys27.tex | |
parent | eee8a108b8592b23778b642d5785a8ba0773e3bb (diff) | |
download | statphys_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.tex | 27 |
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} |