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authorJaron Kent-Dobias <jaron@kent-dobias.com>2017-02-28 18:00:01 -0500
committerJaron Kent-Dobias <jaron@kent-dobias.com>2017-02-28 18:00:01 -0500
commit330000dcacd34664b2baadbda8e4a4afb57e41ec (patch)
treecc857ac5d240e06179c2f13a4f7584e5f788ceb1
parent64db3e9d23dcbaa2e7728e185c13be4344148a60 (diff)
downloadaps_mm_2017-330000dcacd34664b2baadbda8e4a4afb57e41ec.tar.gz
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changes made
-rw-r--r--aps_mm_2017.aux37
-rw-r--r--aps_mm_2017.log1349
-rw-r--r--aps_mm_2017.nav18
-rw-r--r--aps_mm_2017.out0
-rw-r--r--aps_mm_2017.pdfbin0 -> 88369 bytes
-rw-r--r--aps_mm_2017.snm0
-rw-r--r--aps_mm_2017.synctex.gzbin0 -> 12244 bytes
-rw-r--r--aps_mm_2017.tex91
-rw-r--r--aps_mm_2017.toc1
-rw-r--r--figs/fig1.pdfbin0 -> 7095 bytes
-rw-r--r--gen_figs.nb2706
11 files changed, 4194 insertions, 8 deletions
diff --git a/aps_mm_2017.aux b/aps_mm_2017.aux
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diff --git a/aps_mm_2017.log b/aps_mm_2017.log
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\title{Universal scaling and the essential singularity at the Ising first-order transition}
\author{ Jaron~Kent-Dobias\inst{1} \and James~Sethna\inst{1}}
\institute{\inst{1}Cornell University}
\date{16 March 2016}
-\usepackage[normalem]{ulem}
\begin{document}
\def\dd{\mathrm d}
+\def\im{\mathop{\mathrm{Im}}}
\begin{frame}
- \usefont{T1}{phv}{b}{n}
\titlepage
\end{frame}
+\begin{frame}
+ \frametitle{Renormalization and free energy}
+ Rescale a system by a factor $b$, with couplings $K\to K'$.
+ From John Cardy's \emph{Scaling and Renormalization in Statistical Physics},
+ free energy per site $f$
+ \[
+ f(\{K\})=g(\{K\})+b^{-d}f(\{K'\})
+ \]
+ \begin{quote}
+ However, if we are interested in extracting only the \emph{singular}
+ behavior of $f$, \dots we may obtain a \emph{homogeneous} transformation law for the
+ \emph{singular part} of the free energy $f_s$
+ \[
+ f_s(\{K\})=b^{-d}f_s(\{K'\})
+ \]
+ \end{quote}
+ Defense: $g(\{K\})$ is an analytic function of $\{K\}$, while the singular
+ part is nonanalytic
+\end{frame}
+
+\begin{frame}
+ Follow thermodynamic functions onto metastable branch.
+\end{frame}
+
+\begin{frame}
+ \[\Delta f\sim\Sigma\gamma(N)-HMN\]
+ Near the critical point, $\gamma(N)\sim N^{\frac{d-1}d}$
+ \[
+ M=|t|^\beta\mathcal M(h/{t^{\beta\delta}})
+ \]
+ \[
+ N_{crit}\sim\bigg(\frac{\Sigma}{HM}\Big(1-\tfrac1d\Big)\bigg)^d
+ \]
+ \[
+ \Delta f_{crit}\sim\Sigma\bigg(\frac{\Sigma}{HM}\bigg)^{d-1}
+ \sim X^{-(d-1)}\frac{\mathcal
+ S^d(X)}{\mathcal M^{d-1}(X)}
+ \]
+ $X=h/t^{\beta\delta}$
+ The probability that such a domain forms and the metastable state decays is given by the Boltzmann factor,
+ so that
+ $\Sigma\sim|t|^\mu$, $\mu=-\nu+\gamma+2\beta$
+ \[
+ \im f\sim e^{-\beta\, \Delta f_{crit}}
+ \sim\mathcal F(X)e^{-1/X^{d-1}}
+ \]
+\end{frame}
+
+\begin{frame}
+ $e^{-1/x}$ is nonanalytic at $x=0$: all derivatives vanish, means that free
+ energy (which has no imaginary part in stable phase) is smooth
+
+ \centering
+ \includegraphics[width=0.7\textwidth]{figs/fig1}
+\end{frame}
+\begin{frame}
+ Analyticity of $F$ means that the imaginary
+
+ \[
+ f(h)=\sum_n A_nh^N
+ \]
+ \[
+ A_n=(-B)^{1-n}\Gamma(n-1)
+ \]
+
+ \[
+ f(h)=\frac1\pi\int_{h'<0}\frac{\dd h'\,\im f(h')}{h'-h}
+ \]
+\end{frame}
+
+\begin{frame}
+ Field theorists (Lubensky, blah blah blah)
+ \[
+ \mathcal
+ \]
+\end{frame}
\end{document}
diff --git a/aps_mm_2017.toc b/aps_mm_2017.toc
new file mode 100644
index 0000000..ae73954
--- /dev/null
+++ b/aps_mm_2017.toc
@@ -0,0 +1 @@
+\beamer@endinputifotherversion {3.36pt}
diff --git a/figs/fig1.pdf b/figs/fig1.pdf
new file mode 100644
index 0000000..2ecae6b
--- /dev/null
+++ b/figs/fig1.pdf
Binary files differ
diff --git a/gen_figs.nb b/gen_figs.nb
new file mode 100644
index 0000000..4d49987
--- /dev/null
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