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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-03-29 15:43:13 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-03-29 15:43:13 +0200 |
commit | 8a0c4b50f2ac99b3c1ab12871fa1811c4d01d569 (patch) | |
tree | 91a5726cb7602acde01d888ab3ef13efe830a581 /stokes.tex | |
parent | b008d32d061c1fe729b04040d099623eb275753f (diff) | |
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Added paragraph to the numerics section.
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-rw-r--r-- | stokes.tex | 11 |
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@@ -1845,6 +1845,17 @@ gapped minima are unlikely to see Stokes lines. } \label{fig:numeric.angle.gap} \end{figure} +We can also see that as the empirical gap is increased, Stokes points tend to +occur at very large phases. This can be seen for $N=32$ in +Fig.~\ref{fig:numeric.angle.gap}, which shows the probability distribution of +Stokes lines discovered as a function of phase $|\theta|$ necessary to reach +them. The curves are broken into sets representing different bins of the +empirical gap $|\lambda_\textrm{min}|$. As the empirical gap grows, Stokes +points become depleted around small phases and concentrate on very large ones. +This supports the idea that around the gapped minima, Stokes points will be +concentrated at phases that are nearly $180^\circ$, where the two-replica +calculation shows that almost all of their nearest neighbors will lie. + \subsection{Pure {\it p}-spin: is analytic continuation possible?} After this work, one is motivated to ask: can analytic continuation be done in |