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-rw-r--r--ising_scaling.tex2
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@@ -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