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authorJaron Kent-Dobias <jaron@kent-dobias.com>2023-05-28 12:21:56 +0200
committerJaron Kent-Dobias <jaron@kent-dobias.com>2023-05-28 12:21:56 +0200
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@@ -729,11 +729,11 @@ and a specific realization of the disordered Hamiltonian is
\end{equation}
where the first $\delta$-function keeps the configurations in the tangent
plane, and the second enforces the spherical constraint. We have anticipated
-treating the logarithm with replicas. We are of course interested in
-points $\mathbf s$ that have certain properties: they are stationary points of
-$H$ with given energy density and stability, and fixed overlap from a reference
-configuration $\pmb\sigma$. We therefore average the free energy above over
-such points, giving
+treating the logarithm with replicas. We are interested in points $\mathbf s$
+that have certain properties: they are stationary points of $H$ with given
+energy density and stability, and fixed overlap from a reference configuration
+$\pmb\sigma$. We therefore average the free energy above over such points,
+giving
\begin{equation}
\begin{aligned}
F_H(\beta\mid E_1,\mu_1,q,\pmb\sigma)