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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-06-08 20:23:30 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-06-08 20:23:30 +0200 |
commit | a911b841e06f588e7e8efc40ed26c02f9a288e1f (patch) | |
tree | 51a71373db3653a3b575f5db0a0db37bda7a4619 /frsb_kac_new.tex | |
parent | 244d97f5cb05b89c7ffa742a5a2fcb21e6aadad6 (diff) | |
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Remove Jorge comment already addressed.
Diffstat (limited to 'frsb_kac_new.tex')
-rw-r--r-- | frsb_kac_new.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/frsb_kac_new.tex b/frsb_kac_new.tex index 86e38ba..e6b604e 100644 --- a/frsb_kac_new.tex +++ b/frsb_kac_new.tex @@ -228,7 +228,7 @@ for a Gaussian distribution, and the average over disorder breaks into a product of two independent averages, one for the gradient factor and one for the determinant. The integration of all variables, including the disorder in the last factor, may be restricted to the domain such that the matrix $\partial\partial H(s_a)-\mu I$ has a specified number of negative eigenvalues (the index {\cal{I}} of the saddle), (see Fyodorov \cite{Fyodorov_2007_Replica} for a detailed discussion) } -$\hat \beta$ is a parameter conjugate to the state energies, i.e. playing the role of an inverse temperature for the metastable states. } +{ $\hat \beta$ is a parameter conjugate to the state energies, i.e. playing the role of an inverse temperature for the metastable states. } \begin{equation} \begin{aligned} \overline{\Sigma(\epsilon, \mu)} |