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\documentclass[fleqn,aspectratio=169]{beamer}
\renewcommand\vec[1]{\mathbf{#1}}
\setbeamerfont{title}{family=\bf}
\setbeamerfont{frametitle}{family=\bf}
\setbeamerfont{normal text}{family=\rm}
\setbeamertemplate{navigation symbols}{}
\usepackage{textcomp,rotating}
\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}}
\date{}
\begin{document}
\begin{frame}
\maketitle
\end{frame}
\begin{frame}
\frametitle{Introduction}
\end{frame}
\begin{frame}
\frametitle{Hard sphere cluster flips}
\begin{columns}
\begin{column}{0.5\textwidth}
\begin{enumerate}
\item \alert<2>{Pick a symmetry transformation.}
\item \alert<3>{Pick a seed.}
\item \alert<4>{Transform the seed.}
\item \alert<5>{Identify particles with intersections.}
\item \alert<6>{Transform each intersecting particle.}
\item \alert<7-12>{Repeat 5--6 until exhausted.}
\end{enumerate}
\end{column}
\begin{column}{0.5\textwidth}
\begin{overprint}
\onslide<1>\includegraphics[width=\textwidth]{figs/hard_free_1.pdf}
\onslide<2>\includegraphics[width=\textwidth]{figs/hard_free_2.pdf}
\onslide<3>\includegraphics[width=\textwidth]{figs/hard_free_3.pdf}
\onslide<4>\includegraphics[width=\textwidth]{figs/hard_free_4.pdf}
\onslide<5>\includegraphics[width=\textwidth]{figs/hard_free_5.pdf}
\onslide<6>\includegraphics[width=\textwidth]{figs/hard_free_6.pdf}
\onslide<7>\includegraphics[width=\textwidth]{figs/hard_free_7.pdf}
\onslide<8>\includegraphics[width=\textwidth]{figs/hard_free_8.pdf}
\onslide<9>\includegraphics[width=\textwidth]{figs/hard_free_9.pdf}
\onslide<10>\includegraphics[width=\textwidth]{figs/hard_free_10.pdf}
\onslide<11>\includegraphics[width=\textwidth]{figs/hard_free_11.pdf}
\onslide<12>\includegraphics[width=\textwidth]{figs/hard_free_12.pdf}
\onslide<13>\includegraphics[width=\textwidth]{figs/hard_free_13.pdf}
\end{overprint}
\end{column}
\end{columns}
\end{frame}
\begin{frame}
\frametitle{Softening up}
\begin{columns}
\begin{column}{0.5\textwidth}
\begin{overprint}
\onslide<1>\includegraphics[width=\textwidth]{figs/soft_free_1.pdf}
\onslide<2>\includegraphics[width=\textwidth]{figs/soft_free_2.pdf}
\onslide<3>\includegraphics[width=\textwidth]{figs/soft_free_3.pdf}
\onslide<4>\includegraphics[width=\textwidth]{figs/soft_free_4.pdf}
\onslide<5>\includegraphics[width=\textwidth]{figs/soft_free_5.pdf}
\onslide<6>\includegraphics[width=\textwidth]{figs/soft_free_6.pdf}
\onslide<7>\includegraphics[width=\textwidth]{figs/soft_free_7.pdf}
\onslide<8>\includegraphics[width=\textwidth]{figs/soft_free_8.pdf}
\onslide<9>\includegraphics[width=\textwidth]{figs/soft_free_9.pdf}
\onslide<10>\includegraphics[width=\textwidth]{figs/soft_free_10.pdf}
\onslide<11>\includegraphics[width=\textwidth]{figs/soft_free_11.pdf}
\end{overprint}
\end{column}
\begin{column}{0.5\textwidth}
Interacting particles with pair potential $V$ have `Ising' Hamiltonian
\[
H=\sum_{ij}V_{ij}(\vec r_i, \vec r_j)
\]
\begin{enumerate}
\item \alert<2>{Pick a symmetry transformation.}
\item \alert<3>{Pick a seed.}
\item \alert<4>{Transform the seed.}
\item \alert<5>{Identify particles with $\Delta V_{ij}>0$.}
\item \alert<6>{Transform each particle with probability $1-e^{-\Delta V_{ij}/T}$.}
\item \alert<7-10>{Repeat 5--6 until exhausted.}
\end{enumerate}
\end{column}
\end{columns}
\end{frame}
\begin{frame}
\frametitle{Hard sphere cluster flips with hard potential}
\begin{columns}
\begin{column}{0.5\textwidth}
Hard potential? Treat it like a particle!
\begin{enumerate}
\item \alert<2>{Pick a symmetry transformation.}
\item \alert<3>{Pick a seed.}
\item \alert<4>{Transform the seed.}
\item \alert<5>{Identify `particles' with intersections.}
\item \alert<6>{Transform each intersecting particle.}
\item \alert<7-15>{Repeat 5--6 until exhausted.}
\end{enumerate}
\end{column}
\begin{column}{0.5\textwidth}
\begin{overprint}
\onslide<1>\includegraphics[width=\textwidth]{figs/hard_box_1.pdf}
\onslide<2>\includegraphics[width=\textwidth]{figs/hard_box_2.pdf}
\onslide<3>\includegraphics[width=\textwidth]{figs/hard_box_3.pdf}
\onslide<4>\includegraphics[width=\textwidth]{figs/hard_box_4.pdf}
\onslide<5>\includegraphics[width=\textwidth]{figs/hard_box_5.pdf}
\onslide<6>\includegraphics[width=\textwidth]{figs/hard_box_6.pdf}
\onslide<7>\includegraphics[width=\textwidth]{figs/hard_box_7.pdf}
\onslide<8>\includegraphics[width=\textwidth]{figs/hard_box_8.pdf}
\onslide<9>\includegraphics[width=\textwidth]{figs/hard_box_9.pdf}
\onslide<10>\includegraphics[width=\textwidth]{figs/hard_box_10.pdf}
\onslide<11>\includegraphics[width=\textwidth]{figs/hard_box_11.pdf}
\onslide<12>\includegraphics[width=\textwidth]{figs/hard_box_12.pdf}
\onslide<13>\includegraphics[width=\textwidth]{figs/hard_box_13.pdf}
\onslide<14>\includegraphics[width=\textwidth]{figs/hard_box_14.pdf}
\onslide<15>\includegraphics[width=\textwidth]{figs/hard_box_50.pdf}
\onslide<16>\includegraphics[width=\textwidth]{figs/hard_box_51.pdf}
\end{overprint}
\end{column}
\end{columns}
\end{frame}
\begin{frame}
\frametitle{Cluster flips with soft potential}
\begin{columns}
\begin{column}{0.5\textwidth}
Soft potential? Treat it like a (big, soft, asymmetric) particle with effective pair potential $\tilde V$!
\begin{enumerate}
\item \alert<2>{Pick a symmetry transformation.}
\item \alert<3>{Pick a seed.}
\item \alert<4>{Transform the seed.}
\item \alert<5>{Identify `particles' with $\Delta\tilde V_{ij}>0$.}
\item \alert<6>{Transform each `particle' with probability $1-e^{-\Delta\tilde V_{ij}/T}$.}
\item \alert<7-15>{Repeat 5--6 until exhausted.}
\end{enumerate}
\end{column}
\begin{column}{0.5\textwidth}
\end{column}
\end{columns}
\end{frame}
\begin{frame}
\frametitle{Cluster flips with soft potential}
\begin{columns}
\begin{column}{0.5\textwidth}
Soft potential? Treat it like a (big, soft, asymmetric) particle transformed to $r_0$!
\end{column}
\begin{column}{0.5\textwidth}
\end{column}
\end{columns}
\end{frame}
\begin{frame}
\frametitle{Caveats \& improvements}
Symmetries of the torus versus all space
Choice of reflection plane important
We can do better with free space!
\end{frame}
\begin{frame}
\frametitle{A better swap?}
\end{frame}
\begin{frame}
\frametitle{Demo time}
\end{frame}
\begin{frame}
\frametitle{The dirty deets}
System with symmetry group $G$ and objects with state $s_i$ (including position, radius, orientation, spin, \dots)
\[
H=\sum_{ij}V(s_i, s_j)+\sum_iU(s_i)
\]
For $s_0\in G$ and new potential $\tilde V$ defined by $\tilde V_{0i}=U(s_0^{-1}\cdot s_i)$,
\begin{align*}
\tilde H&=\sum_{ij}V_{ij}(s_i, s_j)+\sum_iU_i(s_0^{-1}\cdot s_i) \\
&=\sum_{ij}\tilde V_{ij}(s_i, s_j)
\end{align*}
has the form of a system without a potential.
\end{frame}
\end{document}
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