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| -rw-r--r-- | frsb_kac_new.tex | 2 |
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diff --git a/frsb_kac_new.tex b/frsb_kac_new.tex index 514fda9..c2e5eb9 100644 --- a/frsb_kac_new.tex +++ b/frsb_kac_new.tex @@ -220,8 +220,6 @@ 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) } -{\bf Jaron: I think it is better to call $\hat \epsilon \rightarrow \hat \beta$ and add the phrase: - $\hat \beta$ 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} |