P. Gaspard et Jr. Dorfman, CHAOTIC SCATTERING-THEORY, THERMODYNAMIC FORMALISM, AND TRANSPORT-COEFFICIENTS, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 52(4), 1995, pp. 3525-3552
The foundations of the chaotic scattering theory for transport and rea
ction-rate coefficients for classical many-body systems are considered
here in some detail. The thermodynamic formalism of Sinai, Ruelle,and
Bowen [D. Ruelle, Thermodynamic Formalism (Addison-Wesley, Reading, M
A, 1978)] is employed to obtain an expression for the escape rate for
a phase-space trajectory of a system to leave a finite region of phase
space for the first time. This expression relates the escape rate to
the difference between the sum of the positive Lyapunov exponents and
the Kolmogorov-Sinai entropy for the fractal set of phase-space trajec
tories that are trapped forever in the finite region. This relation is
well known for systems of a few degrees of freedom and is extended he
re to systems with many degrees of freedom. The formalism is applied t
o smooth hyperbolic systems, to cellular-automata lattice gases, and t
o hard-sphere systems. In the last case, the geometric constructions o
f Sinai and co-workers [Russ. Math. Surv. 25, 137 (1970); 42, 181 (198
7)] for billiard systems are used to describe the relevant chaotic sca
ttering phenomena. Some applications of this formalism to nonhyperboli
c systems are also discussed.