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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-10-12 17:13:33 +0200 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-10-12 17:13:33 +0200 |
| commit | 87bbba7046c8550fd5c3992e5d43bda53d04f767 (patch) | |
| tree | 7e3c979c58cd4302319faa6b642404adbcf4da02 /ising_scaling.tex | |
| parent | 1b15f980bc16ef3abeb456fe214584f80bff88eb (diff) | |
| download | paper-87bbba7046c8550fd5c3992e5d43bda53d04f767.tar.gz paper-87bbba7046c8550fd5c3992e5d43bda53d04f767.tar.bz2 paper-87bbba7046c8550fd5c3992e5d43bda53d04f767.zip | |
Tweak subsection to section.
Diffstat (limited to 'ising_scaling.tex')
| -rw-r--r-- | ising_scaling.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/ising_scaling.tex b/ising_scaling.tex index 2c540e6..aea42d0 100644 --- a/ising_scaling.tex +++ b/ising_scaling.tex @@ -334,7 +334,7 @@ The location $\theta_c$ is not fixed by any principle and will be left a floatin } \label{fig:schofield.singularities} \end{figure} -\subsection{Functional form for the parametric free energy} +\section{Functional form for the parametric free energy} As we have seen in the previous sections, the unavoidable singularities in the scaling functions are readily expressed as singular functions in the imaginary |