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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-10-18 15:26:47 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-10-18 15:26:47 +0200 |
commit | d86bec539669a0bba67e09f61b3691ba3ff67933 (patch) | |
tree | 8a29367aa9e6df7a7ef65496ac1f87be5fabecf0 /ising_scaling.tex | |
parent | 8e1f4cd5dd4294cc4d09b624f9baad5214b40fc4 (diff) | |
download | paper-d86bec539669a0bba67e09f61b3691ba3ff67933.tar.gz paper-d86bec539669a0bba67e09f61b3691ba3ff67933.tar.bz2 paper-d86bec539669a0bba67e09f61b3691ba3ff67933.zip |
Bit of writing.
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-rw-r--r-- | ising_scaling.tex | 8 |
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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 |