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authorJaron Kent-Dobias <jaron@kent-dobias.com>2021-10-18 15:26:47 +0200
committerJaron Kent-Dobias <jaron@kent-dobias.com>2021-10-18 15:26:47 +0200
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Bit of writing.
-rw-r--r--ising_scaling.tex8
1 files changed, 8 insertions, 0 deletions
diff --git a/ising_scaling.tex b/ising_scaling.tex
index 47b58ec..2301e73 100644
--- a/ising_scaling.tex
+++ b/ising_scaling.tex
@@ -487,6 +487,14 @@ For $\theta>\theta_c$,
\end{equation}
fixing $B$ and $F_c$. Since $A$ and $\tilde B$ are known exactly, these forms can be substituted.
+This leaves as unknown variables the positions $\theta_0$ and
+$\theta_{\mathrm{YL}}$ of the abrupt transition and Yang--Lee edge singularity,
+the amplitude $A_\mathrm{YL}$ of the latter, and the unknown functions $F$ and
+$h$. We determine these approximately by iteration in the polynomial order at
+which the free energy and its derivative matches known results. Gradients can be computed with
+
+A Levenburg--Marquardt algorithm is performed
+
\begin{table}
\begin{tabular}{c|ccc}
$n$ & $\mathcal F_-^{(n)}$ & $\mathcal F_0^{(n)}$ & $\mathcal F_+^{(n)}$ \\\hline