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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-12-07 17:00:38 +0100 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-12-07 17:00:38 +0100 |
commit | fbb4ec482ce847c6590a98876e9df63a4e3a8283 (patch) | |
tree | a4cf1631e7940e9a4cc0aa5517cb3ae3c659280f | |
parent | bc8dc51857c5e4bb8f9722bd476e8a18436f20a6 (diff) | |
parent | e173cb736bc07937d61564f303eab5d0b60f62ed (diff) | |
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Merge branch 'master' of https://git.overleaf.com/5fcce4736e7f601ffb7e1484
-rw-r--r-- | bezout.tex | 11 |
1 files changed, 8 insertions, 3 deletions
@@ -91,9 +91,14 @@ points it has is given by the usual Kac--Rice formula: \partial_y\partial_x\mathop{\mathrm{Re}}H & \partial_y\partial_y\mathop{\mathrm{Re}}H \end{bmatrix}\right|. \end{equation} -This expression is to be averaged over the $J$'s as -$\Sigma= -\overline{\ln \mathcal N_J} = \int dJ \; \ln N_J$, a calculation that involves the replica trick. In +{\color{red} {\bf perhaps not here} This expression is to be averaged over the $J$'s as +$N \Sigma= +\overline{\ln \mathcal N_J} = \int dJ \; \ln N_J$, 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 propert + +} The Cauchy--Riemann relations imply that the matrix is of the form: \begin{equation} \label{eq:real.kac-rice1} |