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author | kurchan.jorge <kurchan.jorge@gmail.com> | 2023-01-23 10:40:15 +0000 |
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committer | node <node@git-bridge-prod-0> | 2023-01-23 10:55:10 +0000 |
commit | 148b89a29e563e104f6681716d23a2111bebf4a5 (patch) | |
tree | 84a81f63f444a40da1d9283eb349ef9f9ee0263a /frsb_kac-rice_letter.tex | |
parent | 3df1436bf703bc9ab05f72f16cbd54a7a0dfb693 (diff) | |
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Update on Overleaf.
Diffstat (limited to 'frsb_kac-rice_letter.tex')
-rw-r--r-- | frsb_kac-rice_letter.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/frsb_kac-rice_letter.tex b/frsb_kac-rice_letter.tex index f41e8ca..b6e7b8b 100644 --- a/frsb_kac-rice_letter.tex +++ b/frsb_kac-rice_letter.tex @@ -32,7 +32,7 @@ The annealed approximation is by now well understood, but is exact for a restricted subset of these problems. Here we derive the exact quenched solution for the general case, which incorporates Parisi's solution for the ground state, as it should. More importantly, including - replica symmetry breaking uncovers the full organization of saddles in terms of their energies and stabilities, a structure that is lost in the annealed approximation. This structure should be a guide for the identification + replica symmetry breaking uncovers the full distribution of saddles at given energy in terms of their stabilities, a structure that is lost in the annealed approximation. This structure should be a guide for the identification of relevant activated processes in relaxational or driven dynamics.} %These examples demonstrate the consistency of the %solution and reveal that the signature of replica symmetry breaking at high |