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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 |