Thermalization without chaos in harmonic systems
arXiv:2110.14551 · doi:10.1016/j.physa.2022.127581
Abstract
Recent numerical results showed that thermalization of Fourier modes is achieved in short time-scales in the Toda model, despite its integrability and the absence of chaos. Here we provide numerical evidence that the scenario according to which chaos is irrelevant for thermalization is realized even in the simplest of all classical integrable system: the harmonic chain. We study relaxation from an atypical condition given with respect to "random" modes, showing that a thermal state with equilibrium properties is attained in short times. Such a result is independent from the orthonormal base used to represent the chain state, provided it is random.
arXiv comment8 pages, 5 figures
References in corpus (27)
- From Quantum Chaos and Eigenstate Thermalization to Statistical Mechanics and Thermodynamics
- Energy flow, partial equilibration and effective temperatures in systems with slow dynamics
- Canonical Typicality
- Generalized Gibbs ensemble in integrable lattice models
- The approach to thermal equilibrium in quantized chaotic systems
- Proof of the Ergodic Theorem and the H-Theorem in Quantum Mechanics
- Effective thermal dynamics following a quantum quench in a spin chain
- Replica Field Theory for Deterministic Models (II): A Non-Random Spin Glass with Glassy Behavior
- A route to thermalization in the -Fermi-Pasta-Ulam system
- Replica Field Theory for Deterministic Models: Binary Sequences with Low Autocorrelation
- q-Breathers and the Fermi-Pasta-Ulam Problem
- Intermittent many-body dynamics at equilibrium
- Equilibration Properties of Classical Integrable Field Theories
- Generalized Gibbs Ensembles of the classical Toda chain
- Macroscopic and Microscopic Thermal Equilibrium
- Statistical mechanics of an integrable system
- Exact out-of-equilibrium steady states in the semiclassical limit of the interacting Bose gas
- Quantum bounds and fluctuation-dissipation relations
- Entropy growth during free expansion of an ideal gas
- Quenched dynamics of classical isolated systems: the spherical spin model with two-body random interactions or the Neumann integrable model
- Thermalization of local observables in the -FPUT chain
- Equilibrium and Dynamics of a Multi-Bath Sherrington-Kirkpatrick Model
- Pre-asymptotic dynamics of the infinite size Neumann (p=2 spherical) model
- Any Orthonormal Basis in High Dimension is Uniformly Distributed over the Sphere
- Temperature dependence of normal mode reconstructions of protein dynamics
- (Non equilibrium) Thermodynamics of Integrable models: The Generalized Gibbs Ensemble description of the classical Neumann Model
- Statistical Features of High-Dimensional Hamiltonian Systems
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- Ergodic observables in non-ergodic systems: the example of the harmonic chain
- Long-time relaxation of a finite spin bath linearly coupled to a qubit
- On the foundations of statistical mechanics
- Open-system eigenstate thermalization in a noninteracting integrable model
- Symplectic Quantization: numerical results for the Feynman propagator on a 1+1 lattice and the theoretical relation with Quantum Field Theory
- Thermalization is typical in large classical and quantum harmonic systems
- Generalised Gibbs Ensemble for spherically constrained harmonic models