{ "id": "cond-mat/0312500", "version": "v1", "published": "2003-12-18T21:31:18.000Z", "updated": "2003-12-18T21:31:18.000Z", "title": "Dynamical scenario for nonextensive statistical mechanics", "authors": [ "Constantino Tsallis" ], "comment": "Invited paper at the Second Sardinian International Conference on \"News and Expectations in Thermostatistics\" held in Villasimius (Cagliari)- Italy in 21-28 September 2003. 12 pages including 2 figures", "doi": "10.1016/j.physa.2004.03.072", "categories": [ "cond-mat.stat-mech" ], "abstract": "Statistical mechanics can only be ultimately justified in terms of microscopic dynamics (classical, quantum, relativistic, or any other). It is known that Boltzmann-Gibbs statistics is based on the hypothesis of exponential sensitivity to the initial conditions, mixing and ergodicity in Gibbs $\\Gamma$-space. What are the corresponding hypothesis for nonextensive statistical mechanics? A scenario for answering such question is advanced, which naturally includes the {\\it a priori} determination of the entropic index $q$, as well as its cause and manifestations, for say many-body Hamiltonian systems, in (i) sensitivity to the initial conditions in Gibbs $\\Gamma$-space, (ii) relaxation of macroscopic quantities towards their values in anomalous stationary states that differ from the usual thermal equilibrium (e.g., in some classes of metastable or quasi-stationary states), and (iii) energy distribution in the $\\Gamma$-space for the same anomalous stationary states.", "revisions": [ { "version": "v1", "updated": "2003-12-18T21:31:18.000Z" } ], "analyses": { "keywords": [ "nonextensive statistical mechanics", "dynamical scenario", "anomalous stationary states", "initial conditions", "many-body hamiltonian systems" ], "tags": [ "conference paper", "journal article" ], "note": { "typesetting": "TeX", "pages": 12, "language": "en", "license": "arXiv", "status": "editable" } } }