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author | jps6 <jps6@cornell.edu> | 2021-10-28 12:29:27 +0000 |
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committer | node <node@git-bridge-prod-0> | 2021-10-28 12:29:28 +0000 |
commit | b433f56fdab96acf9c9e4f491ca330a9c4dfb059 (patch) | |
tree | 80f469df7858cdf8900d5a9cc393d519a8dc4dd3 /ising_scaling.tex | |
parent | a74244b4052cb3e84d927b5c7d500e04f2be77c0 (diff) | |
download | paper-b433f56fdab96acf9c9e4f491ca330a9c4dfb059.tar.gz paper-b433f56fdab96acf9c9e4f491ca330a9c4dfb059.tar.bz2 paper-b433f56fdab96acf9c9e4f491ca330a9c4dfb059.zip |
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-rw-r--r-- | ising_scaling.tex | 2 |
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diff --git a/ising_scaling.tex b/ising_scaling.tex index fb01780..9ef0388 100644 --- a/ising_scaling.tex +++ b/ising_scaling.tex @@ -589,7 +589,7 @@ The scaling function has a number of free parameters: the position $\theta_0$ of the abrupt transition, prefactors in front of singular functions from the abrupt transition and the Yang--Lee point, the coefficients in the analytic part $G$ of the scaling function, and the coefficients in the undetermined -coordinate function $g$. The other parameters $B$, $C_0$, $\theta_{YL$ are determined by known properties. +coordinate function $g$. The other parameters $B$, $C_0$, $\theta_{YL}$ are determined by known properties. For $\theta>\theta_0$, the form \eqref{eq:essential.singularity} can be expanded around $\theta=\theta_0$ to yield |