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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2025-09-09 10:58:46 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2025-09-09 10:58:46 +0200 |
commit | dfb3531e89dedaac2646a09853e85805002f43de (patch) | |
tree | 0176313e60ca2f55b015d9da50723866dd28c519 /zif.tex | |
parent | 9d1b29fcf084f83d7a1d56c0c848abbae32023b0 (diff) | |
download | zif-master.tar.gz zif-master.tar.bz2 zif-master.zip |
Diffstat (limited to 'zif.tex')
-rw-r--r-- | zif.tex | 25 |
1 files changed, 23 insertions, 2 deletions
@@ -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} |