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author | kurchan.jorge <kurchan.jorge@gmail.com> | 2020-12-07 16:02:07 +0000 |
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committer | overleaf <overleaf@localhost> | 2020-12-07 16:02:20 +0000 |
commit | 075968fa95bd2ba34f14e52b0671ae558cd45ce9 (patch) | |
tree | e8e5b1b0b6388715dbccc554cb1bf2ea09a7b2d1 | |
parent | 1f2b3de07c9a8b39e32f621b07ee5e19895e46b9 (diff) | |
download | PRR_3_023064-075968fa95bd2ba34f14e52b0671ae558cd45ce9.tar.gz PRR_3_023064-075968fa95bd2ba34f14e52b0671ae558cd45ce9.tar.bz2 PRR_3_023064-075968fa95bd2ba34f14e52b0671ae558cd45ce9.zip |
Update on Overleaf.
-rw-r--r-- | bezout.tex | 3 |
1 files changed, 2 insertions, 1 deletions
@@ -96,7 +96,8 @@ $N \Sigma= \overline{\ln \mathcal N_J} = \int dJ \; \ln N_J$, a calculation that involves the replica trick. In most, but not all, of the parameter-space that we shall study here, the {\em annealed approximation} $N \Sigma \sim \ln \overline{ \mathcal N_J} = \ln \int dJ \; N_J$ is exact. -A useful property +A useful property of the Gaussian distributions is that gradient and Hessian may be seen to be independent \cite{BrayDean,Fyodorov}, +so that we may treat the delta-functions and the hessians as independent } |