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author | jps6 <jps6@cornell.edu> | 2021-10-28 12:29:59 +0000 |
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committer | node <node@git-bridge-prod-0> | 2021-10-28 12:30:04 +0000 |
commit | e2ae1e1586e23ec9c4334d61626f6f9e3ffe9bdc (patch) | |
tree | f39372a141a48f11a1ffd24737f472f989555a12 | |
parent | b433f56fdab96acf9c9e4f491ca330a9c4dfb059 (diff) | |
download | paper-e2ae1e1586e23ec9c4334d61626f6f9e3ffe9bdc.tar.gz paper-e2ae1e1586e23ec9c4334d61626f6f9e3ffe9bdc.tar.bz2 paper-e2ae1e1586e23ec9c4334d61626f6f9e3ffe9bdc.zip |
Update on Overleaf.
-rw-r--r-- | ising_scaling.tex | 3 |
1 files changed, 2 insertions, 1 deletions
diff --git a/ising_scaling.tex b/ising_scaling.tex index 9ef0388..9410c1f 100644 --- a/ising_scaling.tex +++ b/ising_scaling.tex @@ -589,8 +589,9 @@ 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 $B$, $C_0$, $\theta_{YL}$, and $C_{YL}$ are determined by known properties. For $\theta>\theta_0$, the form \eqref{eq:essential.singularity} can be expanded around $\theta=\theta_0$ to yield \begin{equation} |