Equivalence of thermodynamic ensembles through Laplace and Legendre transforms.
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% equivalence of thermodynamic ensembles through Laplace and Legendre transforms\documentclass[tikz]{standalone}\usetikzlibrary{positioning}\begin{document}\begin{tikzpicture}[trafo/.style={midway,font=\tiny}]\def\hd{2}\def\vd{0.5}\node (Zm) at (0,0) {$Z_m(E)$};\node[right=\hd of Zm] (Zc) {$Z_c(\beta)$};\node[right=\hd of Zc] (Zg) {$Z_g(\mu)$};\node[below=\vd of Zm] (Sm) {$\sigma = \frac{S_m}{N}$};\node[below=\vd of Zc] (F) {$f = \frac{F}{N}$};\node[below=\vd of Zg] (O) {$\frac{\Omega}{V}$};\draw[->] (Zm) -- (Sm);\draw[->] (Zc) -- (F);\draw[->] (Zg) -- (O);\draw[->] (Zm) -- (Zc) node[trafo,below] {Laplace in $E$};\draw[->] (Zc) -- (Zg) node[trafo,below] {Laplace in $N$};\draw[->] (Sm) -- (F) node[trafo,above] {Legendre in $\epsilon = \frac{E}{N}$};\draw[->] (F) -- (O) node[trafo,above] {Legendre in $\rho = \frac{N}{V}$};\end{tikzpicture}\end{document}
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See more on the author page of Janosh Riebesell..