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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2023-01-23 12:34:04 +0100 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2023-01-23 12:34:04 +0100 |
| commit | 255cd496d8ba4a115ba670a64c8445a8b9c2f485 (patch) | |
| tree | 97b4ca556532e1c5d0100ed772df25684e53b1f8 | |
| parent | df2fbf0ee2627c67b0212ac6d549a042038abbe7 (diff) | |
| download | PRE_107_064111-255cd496d8ba4a115ba670a64c8445a8b9c2f485.tar.gz PRE_107_064111-255cd496d8ba4a115ba670a64c8445a8b9c2f485.tar.bz2 PRE_107_064111-255cd496d8ba4a115ba670a64c8445a8b9c2f485.zip | |
More small changes.
| -rw-r--r-- | frsb_kac-rice.bib | 2 | ||||
| -rw-r--r-- | response.tex | 7 |
2 files changed, 3 insertions, 6 deletions
diff --git a/frsb_kac-rice.bib b/frsb_kac-rice.bib index 37ffb2d..6a2b5e8 100644 --- a/frsb_kac-rice.bib +++ b/frsb_kac-rice.bib @@ -294,7 +294,7 @@ @article{Crisanti_1995_Thouless-Anderson-Palmer, author = {Crisanti, A. and Sommers, H.-J.}, - title = {Thouless-Anderson-Palmer Approach to the Spherical $p$-Spin Spin Glass Model}, + title = {{Thouless}-{Anderson}-{Palmer} Approach to the Spherical $p$-Spin Spin Glass Model}, journal = {Journal de Physique I}, publisher = {EDP Sciences}, year = {1995}, 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 |