initial commit, text still from old statphys poster

7 files changed, 692 insertions, 0 deletions

diff --git a/.gitmodules b/.gitmodules
new file mode 100644
index 0000000..726c245
--- /dev/null
+++ b/.gitmodules
@@ -0,0 +1,3 @@
+[submodule "paper"]
+	path = paper
+	url = https://git.kent-dobias.com/research/hidden_order/paper
diff --git a/CULogo-red120px.eps b/CULogo-red120px.eps
new file mode 100644
index 0000000..a47cafd
--- /dev/null
+++ b/CULogo-red120px.eps
diff --git a/a0header.ps b/a0header.ps
new file mode 100644
index 0000000..c9d07a1
--- /dev/null
+++ b/a0header.ps
@@ -0,0 +1,4 @@
+%%BeginFeature *PageSize ISOA0/ISO A0
+2 dict dup /PageSize [2594 3370] put dup /ImagingBBox null put
+setpagedevice
+%%EndFeature
diff --git a/a0poster.cls b/a0poster.cls
new file mode 100644
index 0000000..68fa0f6
--- /dev/null
+++ b/a0poster.cls
@@ -0,0 +1,210 @@
+%% 
+%% This is file `a0poster.cls'
+%% 
+%% Copyright (C) 1997-2004 Gerlinde Kettl and Matthias Weiser
+%%
+%% It may be distributed and/or modified under the
+%% conditions of the LaTeX Project Public License, either version 1.2
+%% of this license or (at your option) any later version.
+%% The latest version of this license is in
+%%    http://www.latex-project.org/lppl.txt
+%% and version 1.2 or later is part of all distributions of LaTeX
+%% version 1999/12/01 or later.
+%%
+%% Problems, bugs and comments to 
+%% tex@kettl.de
+%% 
+
+\ProvidesClass{a0poster}[2004/01/31 v1.22b a0poster class (GK, MW)]
+\NeedsTeXFormat{LaTeX2e}[1995/06/01]
+\LoadClass{article}
+
+\newif\ifportrait
+\newif\ifanullb
+\newif\ifanull
+\newif\ifaeins
+\newif\ifazwei
+\newif\ifadrei
+\newif\ifposterdraft
+
+\newcount\xkoord
+\newcount\ykoord
+\newcount\xscale
+\newcount\yscale
+
+\DeclareOption{a0b}{
+\anullbtrue
+\xkoord=2594 % big points (1 bp=1/72 inch)
+\ykoord=3370 % big points (1 bp=1/72 inch)
+\xscale=2
+\yscale=2
+}
+\DeclareOption{a0}{
+\anulltrue\anullbfalse
+\xkoord=2380 % big points (1 bp=1/72 inch)
+\ykoord=3368 % big points (1 bp=1/72 inch)
+\xscale=2
+\yscale=2
+}
+\DeclareOption{a1}{
+\aeinstrue\anullbfalse
+\xkoord=1684 % big points (1 bp=1/72 inch)
+\ykoord=2380 % big points (1 bp=1/72 inch)
+\xscale=3
+\yscale=3
+}
+\DeclareOption{a2}{
+\azweitrue\anullbfalse
+\xkoord=1190 % big points (1 bp=1/72 inch)
+\ykoord=1684 % big points (1 bp=1/72 inch)
+\xscale=4
+\yscale=4
+
+}
+\DeclareOption{a3}{
+\adreitrue\anullbfalse
+\xkoord=842  % big points (1 bp=1/72 inch)
+\ykoord=1190 % big points (1 bp=1/72 inch)
+\xscale=6
+\yscale=6
+}
+\DeclareOption{landscape}{
+\portraitfalse
+}
+\DeclareOption{portrait}{
+\portraittrue
+}
+\DeclareOption{draft}{   %% Just for downward compatibility
+\posterdrafttrue
+}
+\DeclareOption{posterdraft}{ %% To avoid collisions with the graphics package
+\posterdrafttrue
+}
+\DeclareOption{final}{
+\posterdraftfalse
+}
+\DeclareOption*{\PackageWarning{a0poster}{Unknown Option \CurrentOption}}
+\ExecuteOptions{landscape,a0b,final}
+\ProcessOptions\relax
+
+\ifanullb
+   \setlength{\paperwidth}{119cm}
+   \setlength{\paperheight}{87cm}
+   \setlength{\textwidth}{114cm}
+   \setlength{\textheight}{87cm}
+\else\ifanull
+        \setlength{\paperwidth}{118.82cm}
+        \setlength{\paperheight}{83.96cm}
+        \setlength{\textwidth}{114.82cm}
+        \setlength{\textheight}{79.96cm}
+     \else\ifaeins
+             \setlength{\paperwidth}{83.96cm}
+             \setlength{\paperheight}{59.4cm}
+             \setlength{\textwidth}{79.96cm}
+             \setlength{\textheight}{55.4cm}
+          \else\ifazwei
+                  \setlength{\paperwidth}{59.4cm}
+                  \setlength{\paperheight}{41.98cm}
+                  \setlength{\textwidth}{55.4cm}
+                  \setlength{\textheight}{37.98cm}
+               \else\ifadrei
+                       \setlength{\paperwidth}{41.98cm}
+                       \setlength{\paperheight}{29.7cm}
+                       \setlength{\textwidth}{37.98cm}
+                       \setlength{\textheight}{25.7cm}
+                    \else\relax
+                    \fi
+               \fi
+          \fi
+     \fi
+\fi
+
+
+\ifportrait
+   \newdimen\tausch
+   \setlength{\tausch}{\paperwidth}
+   \setlength{\paperwidth}{\paperheight}
+   \setlength{\paperheight}{\tausch}
+   \setlength{\tausch}{\textwidth}
+   \setlength{\textwidth}{\textheight}
+   \setlength{\textheight}{\tausch}
+\else\relax
+\fi
+
+%% Setting proper dimensions for a DIN A0 printer
+
+\setlength{\headheight}{0 cm}
+\setlength{\headsep}{0 cm}
+\setlength{\topmargin}{0 cm}
+\setlength{\oddsidemargin}{0 cm}
+
+\catcode`\%=11
+\newwrite\Ausgabe
+\immediate\openout\Ausgabe=a0header.ps
+\write\Ausgabe{%%BeginFeature *PageSize ISOA0/ISO A0}
+\ifposterdraft\write\Ausgabe{2 dict dup /PageSize [595 842] put dup /ImagingBBox null put}
+\else\write\Ausgabe{2 dict dup /PageSize [\number\xkoord\space \number\ykoord] put dup /ImagingBBox null put}\fi
+\write\Ausgabe{setpagedevice}
+\ifposterdraft\write\Ausgabe{38 84 translate}
+\write\Ausgabe{0.\number\xscale\space 0.\number\yscale\space scale}\else\relax\fi
+\write\Ausgabe{%%EndFeature}
+\closeout\Ausgabe
+\catcode`\%=14
+
+\special{header=./a0header.ps}
+
+\input{a0size.sty}
+
+\renewcommand{\tiny}{\fontsize{12}{14}\selectfont}
+\renewcommand{\scriptsize}{\fontsize{14.4}{18}\selectfont}   
+\renewcommand{\footnotesize}{\fontsize{17.28}{22}\selectfont}
+\renewcommand{\small}{\fontsize{20.74}{25}\selectfont}
+\renewcommand{\normalsize}{\fontsize{24.88}{30}\selectfont}
+\renewcommand{\large}{\fontsize{29.86}{37}\selectfont}
+\renewcommand{\Large}{\fontsize{35.83}{45}\selectfont}
+\renewcommand{\LARGE}{\fontsize{43}{54}\selectfont}
+\renewcommand{\huge}{\fontsize{51.6}{64}\selectfont}
+\renewcommand{\Huge}{\fontsize{61.92}{77}\selectfont}
+\newcommand{\veryHuge}{\fontsize{74.3}{93}\selectfont}
+\newcommand{\VeryHuge}{\fontsize{89.16}{112}\selectfont}
+\newcommand{\VERYHuge}{\fontsize{107}{134}\selectfont}
+
+\setlength\smallskipamount{6pt plus 2pt minus 2pt}
+\setlength\medskipamount{12pt plus 4pt minus 4pt}
+\setlength\bigskipamount{24pt plus 8pt minus 8pt}
+
+\setlength\abovecaptionskip{25pt}
+\setlength\belowcaptionskip{0pt}
+\setlength\abovedisplayskip{25pt plus 6pt minus 15 pt}
+\setlength\abovedisplayshortskip{0pt plus 6pt}
+\setlength\belowdisplayshortskip{13pt plus 7pt minus 6pt}
+\setlength\belowdisplayskip\abovedisplayskip
+
+\normalsize
+
+\AtBeginDocument{
+\ifanullb
+   \ifportrait\special{papersize=91.51cm,120cm}\else\special{papersize=120cm,91.51cm}\fi
+\else\ifanull
+        \ifportrait\special{papersize=83.96cm,118.82cm}\else\special{papersize=118.82cm,83.96cm}\fi
+     \else\ifaeins
+             \ifportrait\special{papersize=59.4cm,83.96cm}\else\special{papersize=83.96cm,59.4cm}\fi
+          \else\ifazwei
+                  \ifportrait\special{papersize=41.98cm,59.4cm}\else\special{papersize=59.4cm,41.98cm}\fi
+               \else\ifadrei
+                      \ifposterdraft
+                       \ifportrait\special{papersize=29.7cm,41.35cm}\else\special{papersize=41.98cm,29.0cm}\fi
+                      \else
+                       \ifportrait\special{papersize=29.7cm,41.98cm}\else\special{papersize=41.98cm,29.7cm}\fi
+                      \fi
+                    \else\relax
+                    \fi
+               \fi
+          \fi
+     \fi
+\fi
+\pagestyle{empty}}
+
+\endinput
+%% 
+%% End of file `a0poster.cls'.
diff --git a/a0size.sty b/a0size.sty
new file mode 100644
index 0000000..b3788c0
--- /dev/null
+++ b/a0size.sty
@@ -0,0 +1,252 @@
+%% 
+%% This is file `a0size.sty' (v1.22b) included in the a0poster package
+%% 
+%% Copyright (C) 1997-2004 Gerlinde Kettl and Matthias Weiser
+%%
+%% It may be distributed and/or modified under the
+%% conditions of the LaTeX Project Public License, either version 1.2
+%% of this license or (at your option) any later version.
+%% The latest version of this license is in
+%%    http://www.latex-project.org/lppl.txt
+%% and version 1.2 or later is part of all distributions of LaTeX
+%% version 1999/12/01 or later.
+%%
+%% Problems, bugs and comments to 
+%% tex@kettl.de
+%% 
+ 
+\ProvidesFile{a0size.sty}[2004/01/31 v1.22b a0poster class (GK, MW)]
+
+\DeclareFontShape{OT1}{cmr}{m}{n}
+   {  <5> <6> <7> <8> <9> <10> <12> gen * cmr
+      <10.95> cmr10
+      <14.4>  cmr12
+      <17.28><20.74><24.88>cmr17
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmr17}{}
+
+\DeclareFontShape{OT1}{cmr}{m}{sl}
+    {
+      <5><6><7>cmsl8%
+      <8> <9> gen * cmsl
+      <10><10.95>cmsl10%
+      <12><14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmsl12}{}
+
+\DeclareFontShape{OT1}{cmr}{m}{it}
+    {
+      <5><6><7>cmti7%
+      <8>cmti8%
+      <9>cmti9%
+      <10><10.95>cmti10%
+      <12><14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmti12}{}
+
+\DeclareFontShape{OT1}{cmr}{m}{sc}
+    {
+      <5><6><7><8><9><10><10.95><12>
+      <14.4><17.28><20.74><24.88> 
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmcsc10}{}
+
+\DeclareFontShape{OT1}{cmr}{m}{ui}
+   {
+      <5><6><7><8><9><10><10.95><12>
+      <14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmu10}{}
+      
+\DeclareFontShape{OT1}{cmr}{b}{n}
+     {
+      <5><6><7><8><9><10><10.95><12>
+      <14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmb10}{}
+
+\DeclareFontShape{OT1}{cmr}{bx}{n}
+   {
+      <5> <6> <7> <8> <9> gen * cmbx
+      <10><10.95> cmbx10
+      <12><14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmbx12}{}
+       
+\DeclareFontShape{OT1}{cmr}{bx}{sl}
+      {
+      <5> <6> <7> <8> <9>
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmbxsl10}{}
+
+\DeclareFontShape{OT1}{cmr}{bx}{it}
+      {
+      <5> <6>  <7>  <8> <9>
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmbxti10}{}
+
+\DeclareFontShape{OT1}{cmss}{m}{n}
+     {
+      <5><6><7><8>cmss8
+      <9>cmss9
+      <10><10.95>cmss10
+      <12><14.4>cmss12
+      <17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmss17}{}
+
+\DeclareFontShape{OT1}{cmss}{m}{sl}
+    {
+      <5><6><7><8>cmssi8 <9> cmssi9
+      <10><10.95>cmssi10
+      <12><14.4>cmssi12
+      <17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmssi17}{}
+
+\DeclareFontShape{OT1}{cmss}{sbc}{n}
+     {
+      <5> <6> <7> <8> <9> cmssdc10
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmssdc10}{}
+
+\DeclareFontShape{OT1}{cmss}{bx}{n}
+     {
+      <5> <6> <7> <8> <9> cmssbx10
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmssbx10}{}
+
+\DeclareFontShape{OT1}{cmtt}{m}{n}
+     {
+      <5><6><7><8>cmtt8 <9> cmtt9
+      <10><10.95>cmtt10
+      <12><14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmtt12}{}
+      
+\DeclareFontShape{OT1}{cmtt}{m}{it}
+     {
+      <5> <6> <7> <8> <9>
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmitt10}{}     
+     
+\DeclareFontShape{OT1}{cmtt}{m}{sl}
+     {
+      <5> <6> <7> <8> <9>
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmsltt10}{}
+     
+\DeclareFontShape{OT1}{cmtt}{m}{sc}
+     {
+      <5> <6> <7> <8> <9>
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmtcsc10}{}     
+
+\DeclareFontShape{OML}{cmm}{m}{it}
+    { <5> <6> <7> <8> <9> gen * cmmi
+      <10><10.95>cmmi10
+      <12><14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmmi12}{}
+
+\DeclareFontShape{OML}{cmm}{b}{it}{%
+      <5> <6> <7> <8> <9> gen * cmmib
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmmib10}{}
+
+
+\DeclareFontShape{OMS}{cmsy}{m}{n}{%
+      <5> <6> <7> <8> <9> <10> gen * cmsy
+      <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmsy10}{}
+
+\DeclareFontShape{OMS}{cmsy}{b}{n}{%
+      <5> <6> <7> <8> <9> gen * cmbsy
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmbsy10}{}
+
+\DeclareFontShape{OMX}{cmex}{m}{n}{%
+      <-8>sfixed * cmex7
+      <8> cmex8
+      <9> cmex9
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88> 
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmex10}{}
+
+\DeclareFontShape{U}{cmr}{m}{n}
+   {  <5> <6> <7> <8> <9> <10> <12> gen * cmr
+      <10.95> cmr10
+      <14.4>  cmr12
+      <17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmr17}{}
+
+\DeclareFontShape{U}{cmr}{m}{sl}
+    {
+      <5><6><7>cmsl8%
+      <8> <9> gen * cmsl
+      <10><10.95>cmsl10%
+      <12><14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmsl12}{}
+
+\DeclareFontShape{U}{cmr}{m}{it}
+    {
+      <5><6><7>cmti7%
+      <8>cmti8%
+      <9>cmti9%
+      <10><10.95>cmti10%
+      <12><14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmti12}{}
+
+\DeclareFontShape{U}{cmr}{m}{sc}
+    {
+      <5><6><7><8><9><10><10.95><12>
+      <14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmcsc10}{}
+
+\DeclareFontShape{U}{cmr}{m}{ui}
+   {
+      <5><6><7><8><9><10><10.95><12>%
+      <14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmu10}{}
+
+\DeclareFontShape{U}{cmr}{b}{n}
+     {
+      <5><6><7><8><9><10><10.95><12>
+      <14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmb10}{}
+
+\DeclareFontShape{U}{cmr}{bx}{n}
+   {
+      <5> <6> <7> <8> <9> gen * cmbx
+      <10><10.95> cmbx10
+      <12><14.4><17.28><20.74><24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmbx12}{}
+
+\DeclareFontShape{U}{cmr}{bx}{sl}
+      {
+      <5> <6> <7> <8> <9>
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88>
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmbxsl10}{}
+
+\DeclareFontShape{U}{cmr}{bx}{it}
+      {
+      <5> <6>  <7>  <8> <9>
+      <10> <10.95> <12> <14.4> <17.28> <20.74> <24.88> 
+      <29.86> <35.83> <43.00> <51.6> <61.92> <74.3> <89.16> <107.0> cmbxti10}{}
+
+%% Copied from exscale.sty
+%% Copyright (C) 1992-1995 Frank Mittelbach and Rainer Sch\"opf,
+%% all rights reserved.
+
+\DeclareSymbolFont{largesymbols}{OMX}{cmex}{m}{n}
+\newdimen\big@size
+\addto@hook\every@math@size{\setbox\z@\vbox{\hbox{$($}\kern\z@}%
+   \global\big@size 1.2\ht\z@}
+\def\bBigg@#1#2{%
+   {\hbox{$\left#2\vcenter to#1\big@size{}\right.\n@space$}}}
+\def\big{\bBigg@\@ne}
+\def\Big{\bBigg@{1.5}}
+\def\bigg{\bBigg@\tw@}
+\def\Bigg{\bBigg@{2.5}}
+
+%% End of copy
+
+\DeclareMathSizes{24.88}{24.88}{20.74}{14.4}
+\DeclareMathSizes{29.86}{29.86}{20.74}{14.4}
+\DeclareMathSizes{35.83}{35.83}{24.88}{17.28}
+\DeclareMathSizes{43.00}{43.00}{35.83}{24.88}
+\DeclareMathSizes{51.6}{51.6}{35.83}{24.88}
+\DeclareMathSizes{61.92}{61.92}{43}{29.86}
+\DeclareMathSizes{74.3}{74.3}{51.6}{35.83}
+\DeclareMathSizes{89.16}{89.16}{61.92}{43}
+\DeclareMathSizes{107}{107}{74.3}{51.6}
+
+%% End of a0size.sty 
diff --git a/paper b/paper
new file mode 160000
+Subproject 8316fb1d85d8e8acca59ca8405483ce10f4e818
diff --git a/poster_aps_mm_2020.tex b/poster_aps_mm_2020.tex
new file mode 100644
index 0000000..7451fff
--- /dev/null
+++ b/poster_aps_mm_2020.tex
@@ -0,0 +1,223 @@
+%
+%  poster_05.2014.tex - description
+%
+%  Created by  on Tue May 13 12:26:55 PDT 2014.
+%  Copyright (c) 2014 pants productions. All rights reserved.
+%
+\documentclass[portrait]{a0poster}
+
+\usepackage[utf8]{inputenc}
+\usepackage[T1]{fontenc}
+\usepackage[]{amsmath}
+\usepackage{amssymb,latexsym,mathtools,multicol,lipsum,wrapfig}
+\usepackage[font=normalsize,labelfont=bf]{caption}
+\usepackage{tgheros}
+\usepackage[helvet]{sfmath}
+\usepackage[export]{adjustbox}
+\renewcommand*\familydefault{\sfdefault}
+
+\mathtoolsset{showonlyrefs=true}
+
+
+\setlength\textwidth{194pc}
+\begin{document}
+
+\setlength\columnseprule{2pt}
+\setlength\columnsep{5pc}
+\renewenvironment{figure}
+  {\par\medskip\noindent\minipage{\linewidth}}
+    {\endminipage\par\medskip}
+
+    \renewcommand\section[1]{
+    \vspace{3pc}
+    \noindent\huge\textbf{#1}\large
+    \vspace{1.5pc}
+  }
+
+  \newcommand\unit[1]{\hat{\vec{#1}}}
+  \renewcommand\vec[1]{\boldsymbol{\mathbf{#1}}}
+  \newcommand\norm[1]{\|#1\|}
+  \def\rr{\rho}
+  \newcommand\abs[1]{|#1|}
+  \def\dd{\mathrm d}
+  \def\rec{\mathrm{rec}}
+\def\CC{{C\kern-.05em\lower-.4ex\hbox{\cpp +\kern-0.05em+}} }
+\font\cpp=cmr24
+\def\max{\mathrm{max}}
+
+  \noindent\hspace{177pc}\includegraphics[width=18pc]{CULogo-red120px.eps}
+  \vspace{-24.5pc}\\
+  \Huge \textbf{Elastic properties of hidden order in URu$_{\text2}$Si$_{\text2}$ are reproduced by\\ staggered nematic order}
+  \bigskip\\
+  \huge \textbf{Jaron~Kent-Dobias, Michael Matty \& Brad J Ramshaw}
+  \vspace{1pc}
+
+
+  \begin{multicols}{2}
+
+    \section{Introduction}
+    \Large
+
+    \begin{wrapfigure}{r}{.25\textwidth}
+      \centering
+      %\includegraphics[width=0.25\textwidth]{imgs/crack.jpg}
+      \caption{Cracking in concrete.}
+    \end{wrapfigure}
+
+    Understanding material cracking and fracture is necessary for
+    understanding the aging and failure of those materials in our buildings
+    and infrastructure.  In ordinary brittle materials like glass, stress at
+    the tip of a crack causes it to quickly and cleanly propagate through the
+    material.  In ductile materials like metals, this stress is reduced by
+    plastic deformation around the crack tip, forming the crack's
+    \textbf{process zone}.  In quasi- (or disordered) brittle materials like
+    concrete, this stress is reduced by opening a complicated network of
+    microcracks in the process zone.  This makes the structure of the
+    quasibrittle process zone and crack propagation
+    difficult to study by ordinary means.
+
+
+    \section{Fuse Networks}
+
+    \begin{wrapfigure}{l}{.25\textwidth}
+      \centering
+      %\includegraphics[width=0.12\textwidth]{imgs/square_network.pdf}
+      %\includegraphics[width=0.12\textwidth]{imgs/square_high_beta.pdf}\\
+      %\includegraphics[width=0.12\textwidth]{imgs/voronoi_network.pdf}
+      %\includegraphics[width=0.12\textwidth]{imgs/voronoi_high_beta.pdf}
+      \captionof{figure}{Contrasting the square (top) and voronoi (bottom) networks.  {\bf Left:} Unbroken fuse networks. {\bf Right:} A
+    fracture surface in each at low disorder ($\beta=10$).}
+      \label{nets}
+    \end{wrapfigure}
+
+    \Large
+
+    We model quasibrittle cracking and fracture using simulations of fuse
+    networks, which are electrical systems of resistive fuses whose random
+    current thresholds $t$ are cumulatively distributed by $t^\beta$.  $\beta$
+    parameterizes the amount of disorder in the system: large
+    $\beta$ corresponds to vanishing disorder, small $\beta$ to very large
+    disorder.  Fracture is performed adiabatically: the fuse whose ratio of
+    current to threshold is largest breaks, and the current across the
+    networks is recomputed.  In order to reduce lattice effects, which become large for
+    small disorder (see Figure \ref{nets}), we use voronoi meshes for our fuse networks.
+
+
+    \section{Homogeneous Scaling}
+
+    \begin{wrapfigure}{r}{0.25\textwidth}
+      \centering
+      %\includegraphics[width=0.25\textwidth]{imgs/ashivni.png}
+      \captionof{figure}{The `phase diagram' for fracture in homogeneous
+      systems.}
+      \label{ashivni}
+    \end{wrapfigure}
+
+    \Large
+
+    The problem of fracture in fuse networks was unresolved until recently.
+    For low disorder, fracture is nucleation-like, similar to that of ordinary
+    brittle systems.  At large disorder, fracture occurs after a very large
+    amount of uncorrelated damage, and appears percolation-like.
+    Sethna and Shekhawat developed a theory which unifies these behaviors with
+    an {\sc rg} crossover at intermediate disorder characterized by mean-field
+    avalanches.  The percolation-like behavior at high disorder was shown to
+    be unstable under course-graining, and therefore any nonzero $\beta$
+    will cause nucleated fracture at a sufficiently large system size (see
+    Figure \ref{ashivni}).
+
+    In unpublished work, Shekhawat and Sethna found a scaling form for the
+    distribution of network strengths $\sigma_\max$, the largest current
+    applied to the network before it has broken.  It is given by
+    \begin{equation}
+      P(\sigma_\max\mid\beta, L,u)=\sigma_\max^{-\tau_\sigma}\mathcal P(\beta
+      L^{1/\nu_f},\sigma_\max L^\delta,uL^{-\Delta/\nu_f})\label{form}
+    \end{equation}
+    where $\tau_\sigma$, $\nu_f$, $\delta$ and $\Delta$ are universal
+    exponents, $L$ is the system size, and $u$ is an irrelevant scaling
+    variable.  
+
+    \begin{figure}
+      \vspace{1pc}
+      \centering
+      %\includegraphics[width=0.325\textwidth]{imgs/voronoi_homo_big.pdf}
+      %\includegraphics[width=0.325\textwidth]{imgs/voronoi_homo_med.pdf}
+      %\includegraphics[width=0.325\textwidth]{imgs/voronoi_homo_lit.pdf}\\
+      \begin{minipage}[c]{0.325\textwidth}\centering$\pmb{\beta=3}$\end{minipage}
+      \begin{minipage}[c]{0.325\textwidth}\centering$\pmb{\beta=0.5}$\end{minipage}
+      \begin{minipage}[c]{0.325\textwidth}\centering$\pmb{\beta=0.03}$\end{minipage}\\
+      \captionof{figure}{Fractured fuse networks at various $\beta$.  Each colored region shows a
+        contiguous cracked cluster.  The black region shows the surface of
+        the spanning crack.}
+      \label{homo}
+      \vspace{1pc}
+    \end{figure}
+
+
+    \section{Scaling in the Process Zone}
+
+    \begin{figure}
+      \centering
+      %\includegraphics[width=0.245\textwidth]{imgs/sample_16.pdf}
+      %\includegraphics[width=0.245\textwidth]{imgs/sample_32.pdf}
+      %\includegraphics[width=0.245\textwidth]{imgs/sample_64.pdf}
+      %\includegraphics[width=0.245\textwidth]{imgs/sample_128.pdf}\\
+      \begin{minipage}[c]{0.245\textwidth}\centering$\pmb{L=16,\;\beta=1.9}$\end{minipage}
+      \begin{minipage}[c]{0.245\textwidth}\centering$\pmb{L=32,\;\beta=1.2}$\end{minipage}
+      \begin{minipage}[c]{0.245\textwidth}\centering$\pmb{L=64,\;\beta=0.78}$\end{minipage}
+      \begin{minipage}[c]{0.245\textwidth}\centering$\pmb{L=128,\;\beta=0.5}$\end{minipage}\\
+      \captionof{figure}{Notched fuse networks at critical stress.  The
+        disorder for each system is tuned so that $\beta L^{1/\nu_f}$ is
+      constant, and the statistics of each should scale trivially.}
+      \vspace{1pc}
+      \label{notches}
+    \end{figure}
+
+    \Large
+    We have made progress for developing a scaling theory of damage and stress
+    in the process zone of quasibrittle cracks.  We have essentially taken the
+    scaling behavior of \eqref{form} as an ansatz for how the corresponding
+    qualities of a critically semi-cracked network should scale.  We have
+    begun demonstrating the validity of this theory.  Figure \ref{notches}
+    shows critically cracked networks at constant $\beta L^{1/\nu_f}$, an
+    invariant scaling combination under this theory.  As can be seen in Figure
+    \ref{collapse}, the disorder-averaged stress profiles caused by each
+    collapses nicely.
+
+    \begin{figure}
+      \centering
+      %\includegraphics[width=0.5\textwidth]{imgs/legends.pdf}\\
+      \vspace{-.5em}
+      %\includegraphics[width=0.505\textwidth,valign=t]{imgs/sample_collapse_1.pdf}\hfill
+      %\includegraphics[width=0.48\textwidth,valign=t]{imgs/sample_collapse_2.pdf}\\
+      \vspace{-.5em}
+
+      \captionof{figure}{Disorder-averaged stress $\sigma$ as a function of
+        distance $x$ from the tip of a critical crack.  $\beta L^{1/\nu_f}$ is
+        constant for each curve.  \textbf{Left:} The unmodified stress.
+        \textbf{Right:} The stress collapsed.}
+      \label{collapse}
+    \end{figure}
+
+    \section{Next Steps}
+
+    \begin{wrapfigure}{r}{0.25\textwidth}
+      \centering
+      \vspace{-2em}
+      %\includegraphics[width=.25\textwidth]{imgs/voronoi_heir.pdf}
+      \captionof{figure}{A hierarchical voronoi lattice.}
+    \end{wrapfigure}
+
+    \Large
+
+    The voronoi networks we are able to generate allow us great flexibility
+    for future multiscale computational modelling.  Once we have hashed out
+    our scaling theory more thoroughly, we plan on using it to probe much
+    larger systems than previously feasible using networks whose fuse density
+    becomes smaller in regions of less importance.  This should allow us to
+    see cleaner stress and damage scaling and cleanly stitch our discrete system to a
+    continuum approximation.
+
+  \end{multicols}
+\end{document}
+