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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2023-05-25 15:48:48 +0200 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2023-05-25 15:48:48 +0200 |
| commit | fd0b72927daa9df68e0f0c83437b1392a18830a5 (patch) | |
| tree | cdd9fe5b996d02ff073dcc4f15f4ec2a3be9c32e /ising_scaling.tex | |
| parent | 8280facaa0ce71199011ebd3101de02c89601798 (diff) | |
| download | paper-fd0b72927daa9df68e0f0c83437b1392a18830a5.tar.gz paper-fd0b72927daa9df68e0f0c83437b1392a18830a5.tar.bz2 paper-fd0b72927daa9df68e0f0c83437b1392a18830a5.zip | |
Draft of referee response complete.
Diffstat (limited to 'ising_scaling.tex')
| -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 d7d2474..00de5e3 100644 --- a/ising_scaling.tex +++ b/ising_scaling.tex @@ -207,7 +207,7 @@ literature \cite{Mangazeev_2010_Scaling, Clement_2019_Respect}. In the low temperature phase, the free energy 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 +analytically continued to negative $h$ \cite{Langer_1967_Theory, Isakov_1984_Nonanalytic}. The origin can be schematically understood to arise from a singularity that exists in the imaginary free energy of the metastable phase of the model. When the equilibrium Ising model with positive magnetization is subjected to a small |