Ian Jauslin
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authorIan Jauslin <jauslin@ias.edu>2018-02-06 19:57:42 +0000
committerIan Jauslin <jauslin@ias.edu>2018-02-06 19:57:42 +0000
commitbfed53d2c76cc0449d2d6ef1963863092fb98d03 (patch)
treef9ab1f9e84474684dcdaa37b8a0743c4fa93c1b6 /Jauslin_Princeton_2018.tex
As presented at Princeton University on 2018-02-06HEADv1.0master
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+\documentclass{ian-presentation}
+
+\usepackage[hidelinks]{hyperref}
+\usepackage{graphicx}
+\usepackage{amssymb}
+\usepackage{dsfont}
+
+\begin{document}
+\pagestyle{empty}
+\hbox{}\vfil
+\bf\Large
+\hfil Crystalline ordering\par
+\smallskip
+\hfil in hard-core lattice particle systems\par
+\vfil
+\large
+\hfil Ian Jauslin
+\normalsize
+\vfil
+\hfil\rm joint with {\bf Joel L. Lebowitz}\par
+\vfil
+arXiv: \vbox{
+ \hbox{\tt \href{http://arxiv.org/abs/1705.02032}{1705.02032}}
+ \hbox{\tt \href{http://arxiv.org/abs/1708.01912}{1708.01912}}
+}
+\hfill{\tt \href{http://ian.jauslin.org}{http://ian.jauslin.org}}
+\eject
+
+\setcounter{page}1
+\pagestyle{plain}
+
+\title{Gas-liquid-crystal}
+\vfill
+\hfil\includegraphics[width=3.0cm]{gas.png}
+\hfil\includegraphics[width=3.0cm]{liquid.png}
+\hfil\includegraphics[width=3.0cm]{crystal.png}
+\vfill\eject
+
+\title{Hard-core lattice particle (HCLP) systems}
+\vfill
+\hfil\includegraphics[width=1.2cm]{diamond.pdf}
+\hfil\includegraphics[width=1.2cm]{cross.pdf}
+\hfil\includegraphics[width=1.2cm]{hexagon.pdf}
+\par
+\vfill
+\hfil\includegraphics[width=0.9cm]{V_triomino.pdf}
+\hfil\includegraphics[width=0.9cm]{T_tetromino.pdf}
+\hfil\includegraphics[width=0.9cm]{L_tetromino.pdf}
+\hfil\includegraphics[width=0.9cm]{P_pentomino.pdf}
+\vfill
+\eject
+
+\title{Non-sliding HCLPs}
+\begin{itemize}
+ \item There exist a {\bf finite} number $\tau$ of tilings $\{\mathcal L_1,\cdots,\mathcal L_\tau\}$ which are \penalty-1000{\bf periodic} and {\bf isometric} to each other.
+\end{itemize}
+\hfil\includegraphics[width=4cm]{cross_packing_l.pdf}
+\hfil\includegraphics[width=4cm]{cross_packing_r.pdf}
+\vfill
+\eject
+
+\title{Non-sliding HCLPs}
+\begin{itemize}
+ \item Defects are {\bf localized}: for every connected particle configuration $X$ that is {\it not} the subset of a close packing and every $Y\supset X$, there is empty space in $Y$ neighboring $X$.
+\end{itemize}
+\vfill
+\hfil\includegraphics[width=2.1cm]{cross_sliding_2.pdf}
+\hfil\includegraphics[width=2.1cm]{cross_sliding_3a.pdf}
+\hfil\includegraphics[width=2.4cm]{cross_sliding_3b.pdf}
+\vfill
+\eject
+
+\title{Observables}
+\begin{itemize}
+ \item Gibbs measure:
+ $$
+ \left<A\right>_{\nu}
+ :=
+ \lim_{\Lambda\to\Lambda_\infty}
+ \frac1{\Xi_{\Lambda,\nu}(z)}
+ \sum_{X\subset\Lambda}A(X)z^{|X|}\mathfrak B_\nu(X)\prod_{x\neq x'\in X}\varphi(x,x')
+ $$
+ \vskip-10pt
+ \begin{itemize}
+ \item $\Lambda$: finite subset of lattice $\Lambda_\infty$.
+ \item $z\geqslant 0$: fugacity.
+ \item $\varphi(x,x')$: hard-core interaction.
+ \item $\mathfrak B_\nu$: boundary condition: favors the $\nu$-th tiling.
+ \end{itemize}
+ \vskip-5pt
+
+ \item Pressure:
+ \vskip-10pt
+ $$
+ p(z):=\lim_{\Lambda\to\Lambda_\infty}\frac1{|\Lambda|}\log\Xi_{\Lambda,\nu}(z).
+ $$
+\end{itemize}
+\vfill\eject
+
+\title{Theorem}
+\begin{itemize}
+ \item $p(z)-\rho_m\log z$ and $\left<\mathds 1_{x_1}\cdots\mathds 1_{x_n}\right>_\nu$ are {\bf analytic} functions of $1/z$ for large values of $z$.
+ \vfill
+
+ \item There are $\tau$ distinct Gibbs states:
+ $$
+ \left<\mathds 1_x\right>_\nu=
+ \left\{\begin{array}{ll}
+ 1+O(y)&\mathrm{\ if\ }x\in\mathcal L_\nu\\[0.3cm]
+ O(y)&\mathrm{\ if\ not}
+ .
+ \end{array}\right.
+ $$
+\end{itemize}
+\vfill
+\eject
+
+\title{Low-fugacity expansion}
+\begin{itemize}
+ \item Formally,
+ $$
+ \frac1{|\Lambda|}\log\Xi_\Lambda(z)
+ =
+ \sum_{k=1}^\infty b_k(\Lambda)z^k
+ $$
+ where, if $Z_\Lambda(k_i)$ denotes the number of configurations with $k_i$ particles, then
+ $$
+ b_k(\Lambda):=\frac1{|\Lambda|}
+ \sum_{j=1}^k\frac{(-1)^{j+1}}j
+ \sum_{\displaystyle\mathop{\scriptstyle k_1,\cdots,k_j\geqslant 1}_{k_1+\cdots+k_j=k}}Z_\Lambda(k_1)\cdots Z_\Lambda(k_j)
+ $$
+\end{itemize}
+\eject
+
+\title{Low-fugacity expansion}
+\begin{itemize}
+ \item Second term:
+ $$
+ b_2(\Lambda)=\frac1{|\Lambda|}\left(Z_\Lambda(2)-\frac12Z_\Lambda^2(1)\right)
+ $$
+ \item $\frac12 Z_\Lambda^2(1)$: counts non-interacting particle configurations.
+ \item $Z_\Lambda(2)$: counts interacting particle configurations.
+ \item The terms of order $|\Lambda|^2$ cancel out!
+\end{itemize}
+\eject
+
+\title{Low-fugacity expansion}
+\begin{itemize}
+ \item \href{http://dx.doi.org/10.1017/S0305004100011191}{[Ursell, 1927]}, \href{http://dx.doi.org/10.1063/1.1749933}{[Mayer, 1937]}: $b_k(\Lambda)\to b_k$.
+ \item \href{http://dx.doi.org/10.1016/0031-9163(62)90198-1}{[Groeneveld, 1962]}, \href{http://dx.doi.org/10.1016/0003-4916(63)90336-1}{[Ruelle, 1963]}, \href{http://dx.doi.org/10.1063/1.1703906}{[Penrose, 1963]}:
+ $$
+ p(z)=\sum_{k=1}^\infty b_kz^k
+ $$
+ which has a positive radius of convergence.
+\end{itemize}
+\eject
+
+\title{High-fugacity expansion}
+\begin{itemize}
+ \item Inverse fugacity $y\equiv z^{-1}$:
+ $$
+ \Xi_\Lambda(z)=
+ z^{N_{\mathrm{max}}}
+ \sum_{X\subset\Lambda}
+ y^{N_{\mathrm{max}}-|X|}\prod_{x\neq x'\in X}\phi(x,x')
+ $$
+\end{itemize}
+\eject
+
+\title{High-fugacity expansion}
+\begin{itemize}
+ \item Formally,
+ $$
+ \frac1{|\Lambda|}\log\Xi_\Lambda
+ =
+ \rho_m\log z
+ +
+ \sum_{k=1}^\infty c_k(\Lambda)y^k
+ +
+ o(1)
+ $$
+ where, if $Q_\Lambda(k_i)$ denotes the number of configurations with $N_{\mathrm{max}}-k_i$ particles, then
+ $$
+ c_k(\Lambda):=\frac1{|\Lambda|}
+ \sum_{j=1}^k\frac{(-1)^{j+1}}{j\tau^j}
+ \sum_{\displaystyle\mathop{\scriptstyle k_1,\cdots,k_j\geqslant 1}_{k_1+\cdots+k_j=k}}Q_\Lambda(k_1)\cdots Q_\Lambda(k_j)
+ $$
+\end{itemize}
+\eject
+
+\title{High-fugacity expansion}
+\vfill
+\hfil\includegraphics[width=2cm]{gf_diamond1.pdf}
+\hfil\includegraphics[width=2.33cm]{gf_diamond2.pdf}
+\par\vfill
+\hfil\includegraphics[width=2.33cm]{gf_diamond3.pdf}
+\vfill\eject
+
+\title{High-fugacity expansion}
+\begin{itemize}
+ \item \href{http://dx.doi.org/10.1063/1.1697217}{[Gaunt, Fisher, 1965]}: diamonds: $c_k(\Lambda)\to c_k$ for $k\leqslant 9$.
+ \item \href{http://dx.doi.org/10.1098/rsta.1988.0077}{[Joyce, 1988]}: hexagons (integrable, \href{http://dx.doi.org/10.1088/0305-4470/13/3/007}{[Baxter, 1980]}).
+ \item \href{http://dx.doi.org/10.1209/epl/i2005-10166-3}{[Eisenberg, Baram, 2005]}: crosses: $c_k(\Lambda)\to c_k$ for $k\leqslant 6$.
+ \item Cannot be done {\it systematically}: there exist counter-examples: e.g. hard $2\times2$ squares on $\mathbb Z^2$:
+ $$
+ c_1(\Lambda)\propto\sqrt{|\Lambda|}
+ $$
+\end{itemize}
+\eject
+
+\title{Holes interact}
+\begin{itemize}
+ \item Total volume of holes: $\in\rho_m^{-1}\mathbb N$.
+\end{itemize}
+\vfill
+\hfil\includegraphics[height=4.5cm]{hole_example_cross.pdf}
+\hfil\includegraphics[height=4.5cm]{hole_example_square.pdf}
+\vfill
+\eject
+
+\title{Non-sliding condition}
+\begin{itemize}
+ \item Distinct defects are decorrelated.
+\end{itemize}
+\vfill
+\hfil\includegraphics[height=5cm]{hole_example_cross_decorrelated.pdf}
+\vfill
+\eject
+
+\title{Gaunt-Fisher configurations}
+\begin{itemize}
+ \item Group together empty space and neighboring particles.
+\end{itemize}
+\vfill
+\hfil\includegraphics[width=2.5cm]{gaunt_fisher2.pdf}
+\hfil\includegraphics[width=4cm]{gaunt_fisher3.pdf}
+\vfill
+\eject
+
+\title{Defect model}
+\vskip-5pt
+\begin{itemize}
+ \item Map particle system to a model of defects:
+ $$
+ \Xi_{\Lambda,\nu}(z)=z^{\rho_m|\Lambda|}\sum_{\underline\gamma\subset\mathfrak C_\nu(\Lambda)}
+ \left(\prod_{\gamma\neq\gamma'\in\underline\gamma}\Phi(\gamma,\gamma')\right)
+ \prod_{\gamma\in\underline\gamma}\zeta_\nu^{(z)}(\gamma)
+ $$
+ \begin{itemize}
+ \item $\Phi$: hard-core repulsion of defects.
+ \item $\zeta_\nu^{(z)}(\gamma)$: activity of defect.
+ \end{itemize}
+ \item The activity of a defect is exponentially small: $\exists\epsilon\ll 1$
+ $$
+ \zeta_\nu^{(z)}(\gamma)<\epsilon^{|\gamma|}
+ $$
+ \vskip-5pt
+ \item Low-fugacity expansion for defects.
+\end{itemize}
+\eject
+
+\title{Crystallization}
+\vfill
+\begin{itemize}
+ \item Peierls argument: in order to have a particle at $x$ that is not compatible with the $\nu$-th perfect packing, it must be part of or surrounded by a defect.
+ \vfill
+ \item Note: a naive Peierls argument requires the partition function to be independent from the boundary condition. This is not necessarily the case here, and we need elements from Pirogov-Sinai theory.
+\end{itemize}
+
+
+\end{document}