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Stability analysis of the entropies for superstatistics

โœ Scribed by Andre M.C. Souza; Constantino Tsallis


Publisher
Elsevier Science
Year
2004
Tongue
English
Weight
206 KB
Volume
342
Category
Article
ISSN
0378-4371

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โœฆ Synopsis


It seems reasonable to consider concavity (with regard to all probability distributions) and stability (under arbitrarily small deformations of any given probability distribution) as necessary for an entropic form to be a physical one in the thermostatistical sense. Most known entropic forms, e.g. Renyi entropy S R q =(ln i p q i )=(1-q), violate one and/or the other of these conditions. In contrast, the Boltzmann-Gibbs entropy SBG =i pi ln pi and the nonextensive one Sq = (1i p q i )=(q -1) (q ยฟ 1) satisfy both. SBG and Sq belong in fact to a larger class of entropies S satisfying both, namely those which, through appropriate optimization, yield the Beck-Cohen superstatistics. We brie y review here the proof of stability of S, and illustrate for an important particular case, namely the log-normal superstatistical entropy. The satisfaction of both concavity and stability appears to be very helpful to identify physically admissible entropic forms.


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Thermodynamic stabilities of the general
โœ Tatsuaki Wada ๐Ÿ“‚ Article ๐Ÿ“… 2004 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 184 KB

We consider the thermodynamic stability conditions (TSC) on the Boltzmann entropies generalized by Tsallis' q-and Kaniadakis' ร„-deformed logarithmic functions. It is shown that the corresponding TSCs are not necessarily equivalent to the concavity of the generalized Boltzmann entropies with respect