Abstract:A statistical system is classically defined on a set of microstates E by a global energy function H : E → R, yielding Gibbs probability measures (softmins) ρ β (H) for every inverse temperature β = T −1 . Gibbs states are simultaneously characterised by free energy principles and the maxentropy principle, with dual constraints on inverse temperature β and mean energy U(β) = E ρ β [H] respectively. The Legendre transform relates these diverse variational principles [1, 2] which are unfortunately not tractable i… Show more
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