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Diffstat (limited to 'response.tex')
| -rw-r--r-- | response.tex | 7 |
1 files changed, 2 insertions, 5 deletions
diff --git a/response.tex b/response.tex index 3454eaf..6abde6c 100644 --- a/response.tex +++ b/response.tex @@ -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 |