Chaos, ergodicity, and the thermodynamics of lower-dimensional Hamiltonian systems
arXiv:astro-ph/0108038 · doi:10.1103/PhysRevE.65.016214
Abstract
This paper uses the assumptions of ergodicity and a microcanonical distribution to compute estimates of the largest Lyapunov exponents in lower-dimensional Hamiltonian systems. That the resulting estimates are in reasonable agreement with the actual values computed numerically corroborates the intuition that chaos in such systems can be understood as arising generically from a parametric instability and that this instability can be modeled by a stochastic-oscillator equation (cf. Casetti, Clementi, and Pettini, Phys. Rev. E 54, 5969 (1996)), linearised perturbations of a chaotic orbit satisfying a harmonic-oscillator equation with a randomly varying frequency.
19 pp. including 14 Figures, uses Phys. Rev. macros
Cited by in corpus (9)
- Transient chaos and resonant phase mixing in violent relaxation
- Phase separation can be stronger than chaos
- Smooth potential chaos and N-body simulations
- Chaotic Orbits in Thermal-Equilibrium Beams: Existence and Dynamical Implications
- Spatial Phase Separation of a Binary Mixture in a Ring Trimer
- Lyapunov exponent of many-particle systems: testing the stochastic approach
- Semi-Analytic Estimates of Lyapunov Exponents in Lower-Dimensional Systems
- Partial suppression of chaos in relativistic three-body problems
- Quantum Field Theory of Classically Unstable Hamiltonian Dynamics