Departure from Boltzmann-Gibbs statistics makes the hydrogen-atom specific heat a computable quantity

Abstract
The specific heat of the (nonionized) hydrogen atom in free space cannot be calculated within Boltzmann-Gibbs statistical mechanics essentially because its partition function diverges. We show that a recently introduced generalized formalism can overcome this difficulty for qq characterizes the statistics; Boltzmann-Gibbs corresponds to q=1).

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