Linear instability and statistical laws of physicsG. Casati1, 2, 3, C. Tsallis4, 5 and F. Baldovin6, 7
1 Center for Nonlinear and Complex Systems, Università degli Studi dell'Insubria Via Valleggio 11, 22100 Como, Italy
2 CNR-INFM, Istituto Nazionale di Fisica Nucleare, Sezione di Milano - Milano, Italy
3 Department of Physics, National University of Singapore Singapore 117542, Republic of Singapore
4 Santa Fe Institute - 1399 Hyde Park Road, Santa Fe, NM 87501, USA
5 Centro Brasileiro de Pesquisas Físicas - Rua Xavier Sigaud 150 22290-180 Rio de Janeiro-RJ, Brazil
6 INFM-Dipartimento di Fisica, Università di Padova Via Marzolo 8, I-35131 Padova, Italy
7 Sezione INFN, Università di Padova - Via Marzolo 8, I-35131 Padova, Italy
received 29 July 2005; accepted 8 September 2005
published online 30 September 2005
We show that a meaningful statistical description is possible in conservative and mixing systems with zero Lyapunov exponent in which the dynamical instability is only linear in time. More specifically, i) the sensitivity to initial conditions is given by with q=0; ii) the statistical entropy in the infinitely fine graining limit (i.e., number of cells into which the phase space has been partitioned ), increases linearly with time only for q=0; iii) a nontrivial, q-generalized, Pesin-like identity is satisfied, namely the . These facts (which are in analogy to the usual behaviour of strongly chaotic systems with q=1), seem to open the door for a statistical description of conservative many-body nonlinear systems whose Lyapunov spectrum vanishes.
05.45.Ac - Low-dimensional chaos.
05.45.Mt - Quantum chaos; semiclassical methods.
03.67.Lx - Quantum computation.
© EDP Sciences 2005