From d657f2a2edaa39f8f3545d6ac71e6a63b22faeba Mon Sep 17 00:00:00 2001 From: jps6 Date: Tue, 10 Aug 2021 15:09:49 +0000 Subject: Update on Overleaf. --- ising_scaling.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) 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 -- cgit v1.2.3-70-g09d2