{ "id": "cond-mat/9907412", "version": "v4", "published": "1999-07-27T08:18:06.000Z", "updated": "2000-07-07T15:32:42.000Z", "title": "The rate of entropy increase at the edge of chaos", "authors": [ "V. Latora", "M. Baranger", "A. Rapisarda", "C. Tsallis" ], "comment": "6 pages, Latex, 4 figures included, final version accepted for publication in Physics Letters A", "journal": "Phys.Lett. A273 (2000) 97", "doi": "10.1016/S0375-9601(00)00484-9", "categories": [ "cond-mat.stat-mech", "astro-ph", "chao-dyn", "comp-gas", "hep-th", "nlin.CD", "nlin.CG", "nucl-th" ], "abstract": "Under certain conditions, the rate of increase of the statistical entropy of a simple, fully chaotic, conservative system is known to be given by a single number, characteristic of this system, the Kolmogorov-Sinai entropy rate. This connection is here generalized to a simple dissipative system, the logistic map, and especially to the chaos threshold of the latter, the edge of chaos. It is found that, in the edge-of-chaos case, the usual Boltzmann-Gibbs-Shannon entropy is not appropriate. Instead, the non-extensive entropy $S_q\\equiv \\frac{1-\\sum_{i=1}^W p_i^q}{q-1}$, must be used. The latter contains a parameter q, the entropic index which must be given a special value $q^*\\ne 1$ (for q=1 one recovers the usual entropy) characteristic of the edge-of-chaos under consideration. The same q^* enters also in the description of the sensitivity to initial conditions, as well as in that of the multifractal spectrum of the attractor.", "revisions": [ { "version": "v4", "updated": "2000-07-07T15:32:42.000Z" } ], "analyses": { "keywords": [ "entropy increase", "usual boltzmann-gibbs-shannon entropy", "kolmogorov-sinai entropy rate", "initial conditions", "usual entropy" ], "tags": [ "journal article" ], "note": { "typesetting": "LaTeX", "pages": 6, "language": "en", "license": "arXiv", "status": "editable", "inspire": 506399 } } }