Comment on ``Nonextensive hamiltonian systems follow Boltzmann's principle not Tsallis statistics-phase transition, second law of thermodynamics'' by Gross

Physics – Condensed Matter – Statistical Mechanics

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5pages, no figure, Tex

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Recently, Gross claims that Boltzmann entropy $S=k\ln W$ is valid for any
system at equilibrium, so that Tsallis entropy is useless in this case. I
comment on some arguments forwarded to reach this conclusion and argue that the
additive energy formalism of nonextensive statistics is not appropriate for the
fundamental study of the theory for nonadditive systems.

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