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authorJaron Kent-Dobias <jaron@kent-dobias.com>2025-09-09 10:58:46 +0200
committerJaron Kent-Dobias <jaron@kent-dobias.com>2025-09-09 10:58:46 +0200
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-rw-r--r--zif.tex25
1 files changed, 23 insertions, 2 deletions
diff --git a/zif.tex b/zif.tex
index 50f083f..38aa2c4 100644
--- a/zif.tex
+++ b/zif.tex
@@ -158,9 +158,11 @@
\#_\text{points}
&=\int_\Omega d\boldsymbol x\,\delta\big(\nabla H(\boldsymbol x)\big)\,\big|\det\operatorname{Hess}H(\boldsymbol x)\big|
\end{align*}
- Note absolute value of the determinant: want to account for curvature but not add $-1$
- \bigskip
+ Typically exponential in dimension $N$, with \emph{complexity} defined by
+ \[
+ \Sigma=\frac1N\log\#_\text{points}
+ \]
Can specify properties of points by inserting $\delta$-functions:
\begin{align*}
@@ -1194,6 +1196,25 @@
\end{frame}
\begin{frame}
+ \frametitle{Other landscape applications without RMT}
+
+ \begin{columns}
+ \begin{column}{0.5\textwidth}
+ \includegraphics[width=\textwidth]{figs/folena_new.pdf}
+
+ \tiny\fullcite{Kent-Dobias_2025_On}
+ \end{column}
+ \begin{column}{0.5\textwidth}
+ \vspace{2.5em}
+
+ \includegraphics[width=\textwidth]{figs/walk.pdf}
+
+ \tiny\fullcite{Kent-Dobias_2025_Very}
+ \end{column}
+ \end{columns}
+\end{frame}
+
+\begin{frame}
\frametitle{Understanding the flat parts of random landscapes}
\begin{columns}
\begin{column}{0.33\textwidth}