Introduction to Nonextensive Statistical Mechanics and Thermodynamics
arXiv:cond-mat/0309093
Abstract
In this lecture we briefly review the definition, consequences and applications of an entropy, , which generalizes the usual Boltzmann-Gibbs entropy (), basis of the usual statistical mechanics, well known to be applicable whenever ergodicity is satisfied at the microscopic dynamical level. Such entropy is based on the notion of -exponential and presents properties not shared by other available alternative generalizations of . The thermodynamics proposed in this way is generically {\it nonextensive} in a sense that will be qualified. The present framework seems to describe quite well a vast class of natural and artificial systems which are not ergodic nor close to it. The a priori calculation of is necessary to complete the theory and we present some models where this has already been achieved.
To appear in the Proceedings of the 1953-2003 Jubilee "Enrico Fermi" International Summer School of Physics {\it The Physics of Complex Systems: New Advances & Perspectives}, Directors F. Mallamace and H.E. Stanley (1-11 July 2003, Varenna sul lago di Como). The present manuscript reports the content of the lecture delivered by C. Tsallis, and is based on the corresponding notes prepared by F. Baldovin, R. Cerbino and P. Pierobon, students at the School. 24 pages including 3 figures
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