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| author | kurchan.jorge <kurchan.jorge@gmail.com> | 2020-12-09 15:59:26 +0000 |
|---|---|---|
| committer | overleaf <overleaf@localhost> | 2020-12-09 16:02:22 +0000 |
| commit | 4943c8d5d578396bd3087c1e7609b4973e4532bc (patch) | |
| tree | f43b2c29b700a29d5979b889f87b928d6318118b | |
| parent | 4c7e7edb6c7b74ded74a4437d7b15f32c1e6f378 (diff) | |
| download | PRR_3_023064-4943c8d5d578396bd3087c1e7609b4973e4532bc.tar.gz PRR_3_023064-4943c8d5d578396bd3087c1e7609b4973e4532bc.tar.bz2 PRR_3_023064-4943c8d5d578396bd3087c1e7609b4973e4532bc.zip | |
Update on Overleaf.
| -rw-r--r-- | bezout.tex | 2 |
1 files changed, 1 insertions, 1 deletions
@@ -319,7 +319,7 @@ The number of critical points contained within is =(p-1)^{N/2}, \end{equation} the square root of \eqref{eq:bezout} and precisely the number of critical -points of the real pure spherical $p$-spin model. In fact, the full +points of the real pure spherical $p$-spin model. (note the role of conjugation symmetry, already underlined in Ref\cite{bogomolny1992distribution}). In fact, the full $\epsilon$-dependence of the real pure spherical $p$-spin is recovered by this limit as $\epsilon$ is varied. |