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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2023-11-21 17:38:59 +0100 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2023-11-21 17:38:59 +0100 |
commit | 4fdc2756ff9b2cf29bbe2f21a2db9d9f9040fe54 (patch) | |
tree | 9d45d7ffea947f24bf101b291234354830c64c12 /2-point.tex | |
parent | 35ce3da68e51c95125faaa301957718f5097ea45 (diff) | |
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Made a sentence about marginal minima attracting dynamics more simple
for referee.
Diffstat (limited to '2-point.tex')
-rw-r--r-- | 2-point.tex | 8 |
1 files changed, 4 insertions, 4 deletions
diff --git a/2-point.tex b/2-point.tex index d5ef022..5f9bda8 100644 --- a/2-point.tex +++ b/2-point.tex @@ -429,10 +429,10 @@ lowest-energy states. This is seen in Fig.~\ref{fig:franz-parisi}. The set of marginal states is of special interest. First, it has more structure than in the pure models, with different types of marginal states being found at -different energies. Second, these states attract the dynamics (as evidenced by power-law relaxations), and so are the -inevitable end-point of equilibrium and algorithmic processes \cite{Folena_2023_On}. We find, -surprisingly, that the properties of marginal states pivot around the threshold -energy, the energy at which most stationary points are marginal. +different energies. Second, marginal states are known to attract physical and +algorithmic dynamics \cite{Folena_2023_On}. We find, surprisingly, that the +properties of marginal states pivot around the threshold energy, the energy at +which most stationary points are marginal. \begin{itemize} \item \textbf{Energies below the threshold.} Marginal states have a |