Abstract
It is by now well known that the Boltzmann-Gibbs (BG) entropy can be usefully generalized using the nonextensive entropies, which have been applied to a wide range of phenomena. However, it seems that even more general entropies could be useful in order to describe other complex physical systems, a task which has already been undertaken in the literature. Following this approach, we introduce here a quite general entropy based on a distribution of indices thus generalizing . We establish some general mathematical properties for the new entropic functional and explore some examples. We also exhibit a procedure for finding, given any entropic functional, the -indices distribution that produces it. Finally, on the road to establishing a quite general statistical mechanics, we briefly address possible generalized constraints under which the present entropy could be extremized, in order to produce canonical-ensemble-like stationary-state distributions for Hamiltonian systems.
- Received 13 December 2004
DOI:https://doi.org/10.1103/PhysRevE.71.046144
©2005 American Physical Society