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| author | jps6 <jps6@cornell.edu> | 2021-08-10 15:09:49 +0000 |
|---|---|---|
| committer | node <node@git-bridge-prod-0> | 2021-10-12 14:16:54 +0000 |
| commit | d657f2a2edaa39f8f3545d6ac71e6a63b22faeba (patch) | |
| tree | 5147bb604193f5a38abcd1a6c52eb2f8d5ad61fb | |
| parent | d1cfd572aaadae2a56c117a8b127c61131fc0dd6 (diff) | |
| download | paper-d657f2a2edaa39f8f3545d6ac71e6a63b22faeba.tar.gz paper-d657f2a2edaa39f8f3545d6ac71e6a63b22faeba.tar.bz2 paper-d657f2a2edaa39f8f3545d6ac71e6a63b22faeba.zip | |
Update on Overleaf.
| -rw-r--r-- | ising_scaling.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/ising_scaling.tex b/ising_scaling.tex index c6dc29a..8bc17d7 100644 --- a/ising_scaling.tex +++ b/ising_scaling.tex @@ -148,7 +148,7 @@ models) in the literature \cite{Clement_2019_Respect}. In the low temperature phase, the free energy as a function of field has an essential singularity at zero field, which becomes a branch cut along the negative-$h$ axis when analytically continued to negative $h$ \cite{Langer_1967_Theory}. The origin can be schematically understood to arise from a singularity that exists in the complex free energy of the metastable phase of the model, suitably continued into the equilibrium phase. When the equilibrium -Ising model with positive magnetization is subjected to a small negative +Ising model with positive magnetization is subjehttps://www.overleaf.com/project/601afd459bf8018881b982a3cted to a small negative magnetic field, its equilibrium state instantly becomes one with a negative magnetization. However, under physical dynamics it takes time to arrive at this state, which happens after a fluctuation containing a sufficiently large |