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authorJaron Kent-Dobias <jaron@kent-dobias.com>2023-01-23 12:34:04 +0100
committerJaron Kent-Dobias <jaron@kent-dobias.com>2023-01-23 12:34:04 +0100
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@@ -126,7 +126,7 @@ that "the complexity of the mixed p-spin glass models" is not a major
breakthrough in and of itself, we just
chose to demonstrate the problem in simplest toy model. But believe that the technique for
computing the quenched complexity is a major breakthrough
-{\bf because it brings in the features of organization of saddles of all
+\textit{because it brings in the features of organization of saddles of all
kinds that are invisible in the annealed scheme}.
@@ -168,15 +168,12 @@ The novelty of the paper is most definitely
not the fact of treating a zero temperature case.
We have added the following phrase, that should clarify the situation:
-{\color{blue}
For simplicity we have concentrated here on the energy, rather
than {\em free-energy} landscape, although the latter is sometimes
more appropriate. From the technical point of view, this makes no fundamental difference, it suffices
-to apply the same computation to the Thouless-Andreson-Palmer \cite{Crisanti_1995_Thouless-Anderson-Palmer} (TAP) free energy, instead of the energy. We do not expect new features or technical
+to apply the same computation to the Thouless-Andreson-Palmer (TAP) free energy, \footfullcite{Crisanti_1995_Thouless-Anderson-Palmer} instead of the energy. We do not expect new features or technical
complications arise.
-}
-
%For a system where the quenched and annealed
%complexities differ, there has not been a correct calculation of the