From 2d3bbbe56c6d54fa63d5c39f8122b6c68b6368d4 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Fri, 28 Feb 2020 09:01:13 -0500
Subject: Several changes.

  - New animation for hard sphere flip where the first move looks more
    distinct

  - Colorful Cornell seal

  - Started trimming text to be more succinct
---
 aps_mm_2020.tex | 37 ++++++++++++++++++++++---------------
 1 file changed, 22 insertions(+), 15 deletions(-)

(limited to 'aps_mm_2020.tex')

diff --git a/aps_mm_2020.tex b/aps_mm_2020.tex
index 171b1ed..b97f13b 100644
--- a/aps_mm_2020.tex
+++ b/aps_mm_2020.tex
@@ -12,7 +12,7 @@
 
 \title{Cluster-flip colloidal \& atomistic algorithms with background potentials}
 \author{Jaron Kent-Dobias \and James P Sethna}
-\institute{\includegraphics[width=7em]{figs/bold_cornell_seal_black.pdf}}
+\institute{\includegraphics[width=7em]{figs/bold_cornell_seal_cmyk_red.pdf}}
 \date{}
 
 \begin{document}
@@ -34,28 +34,24 @@
     \begin{column}{0.5\textwidth}
       Cluster Monte Carlo famously speeds up simulation of lattice models.
 
+      \hfill{\scriptsize Wang \& Swendsen, Physica A \textbf{167} (1990) 565}\\
+      \hfill{\scriptsize Wolff, PRL \textbf{62} 4 (1989) 361}
+
       \vspace{1em}
 
       Recent extension for lattice models extends this to arbitrary potentials.
 
-      \hfill{\scriptsize PRE \textbf{98} 063306 (2018)}
+      \hfill{\scriptsize Kent-Dobias \& Sethna, PRE \textbf{98} 063306}
 
       \vspace{1em}
 
       That method also happens to work for spatial degrees of freedom!
-
-      \begin{enumerate}
-        \item Introduce known methods without potentials.
-        \item Introduce new method with potentials.
-        \item Discuss real and speculated improvements.
-        \item Watch some fun demos.
-      \end{enumerate}
     \end{column}
   \end{columns}
 \end{frame}
 
 \begin{frame}
-  \frametitle{Hard sphere cluster flips}
+  \frametitle{Hard spheres without potential}
   
   \begin{columns}
     \begin{column}{0.5\textwidth}
@@ -67,6 +63,10 @@
         \item \alert<6>{Transform each intersecting particle.}
         \item \alert<7-12>{Repeat 5--6 until exhausted.}
       \end{enumerate}
+
+      \vspace{1em}
+
+      \hfill{\scriptsize Dress \& Krauth \textit{J Phys A: Math Gen} \textbf{28} (1995) 597} 
     \end{column}
     \begin{column}{0.5\textwidth}
       \begin{overprint}
@@ -89,7 +89,7 @@
 \end{frame}
 
 \begin{frame}
-  \frametitle{Softening up}
+  \frametitle{Soft spheres without potential}
   \begin{columns}
     \begin{column}{0.5\textwidth}
       \begin{overprint}
@@ -109,7 +109,7 @@
       \end{overprint}
     \end{column}
     \begin{column}{0.5\textwidth}
-      Interacting particles with pair potential $V$ have `Ising' Hamiltonian
+      Pair potential $V$ gives `Ising' Hamiltonian:
       \[
         H=\sum_{ij}V_{ij}(\vec r_i, \vec r_j)
       \]
@@ -128,7 +128,7 @@
 \end{frame}
 
 \begin{frame}
-  \frametitle{Hard sphere cluster flips with hard potential}
+  \frametitle{Spheres in hard potential}
   \begin{columns}
     \begin{column}{0.5\textwidth}
       Hard potential? Treat it like a particle!
@@ -166,10 +166,17 @@
 \end{frame}
 
 \begin{frame}
-  \frametitle{Cluster flips with soft potential}
+  \frametitle{Spheres in soft potential}
   \begin{columns}
     \begin{column}{0.5\textwidth}
-      Soft potential? Treat it like a (big, soft, asymmetric) particle with effective pair potential $\tilde V$!
+      Soft potential? Treat it like a particle with effective pair potential $\tilde V$!
+
+      \vspace{0.5em}
+
+      \raisebox{-0.65em}{\includegraphics[width=0.1\textwidth]{figs/ex.pdf}} --- center of attractive potential
+
+      \vspace{0.5em}
+
       \begin{enumerate}
         \item \alert<2>{Pick a symmetry transformation.}
         \item \alert<3>{Pick a seed.}
-- 
cgit v1.2.3-54-g00ecf