Simulating quantum thermodynamics of a finite system and bath with variable temperature
arXiv:1906.05428 · doi:10.1103/PhysRevE.100.042105
Abstract
We construct a finite bath with variable temperature for quantum thermodynamic simulations in which heat flows between a system and the bath environment in time evolution of an initial pure state. The bath consists of harmonic oscillators that are not necessarily identical. Baths of various numbers of oscillators are considered; a bath with five oscillators is used in the simulations. The bath has a temperature-like level distribution. This leads to definition of a system-environment microcanonical temperature which varies with time. The quantum state evolves toward an equilibrium state which is thermal-like, but there is significant deviation from the ordinary energy-temperature relation that holds for an infinite quantum bath, e.g. an infinite system of identical oscillators. There are also deviations from the Einstein quantum heat capacity. The temperature of the finite bath is systematically greater for a given energy than the infinite bath temperature, and asymptotically approaches the latter as the number of oscillators increases. It is suggested that realizations of these finite-size effects may be attained in computational and experimental dynamics of small molecules.
arXiv comment13 pages, 9 figures
References in corpus (25)
- Thermalization and its mechanism for generic isolated quantum systems
- From Quantum Chaos and Eigenstate Thermalization to Statistical Mechanics and Thermodynamics
- Quantum thermalization through entanglement in an isolated many-body system
- The foundations of statistical mechanics from entanglement: Individual states vs. averages
- Canonical Typicality
- Quantum mechanical evolution towards thermal equilibrium
- Eigenstate Thermalization Hypothesis
- Foundation of Statistical Mechanics under experimentally realistic conditions
- Entropy production as correlation between system and reservoir
- From Quantum Dynamics to the Canonical Distribution: General Picture and a Rigorous Example
- An improved Landauer Principle with finite-size corrections
- Proof of the Ergodic Theorem and the H-Theorem in Quantum Mechanics
- Microscopic diagonal entropy and its connection to basic thermodynamic relations
- Long-Time Behavior of Macroscopic Quantum Systems: Commentary Accompanying the English Translation of John von Neumann's 1929 Article on the Quantum Ergodic Theorem
- On the Approach to Thermal Equilibrium of Macroscopic Quantum Systems
- Quantum Information and Entropy
- Typical fast thermalization processes in closed many-body systems
- Extremely quick thermalization in a macroscopic quantum system for a typical nonequilibrium subspace
- Spin relaxation in a complex environment
- Relaxation into equilibrium under pure Schrödinger dynamics
- Entropy for Quantum Pure States and Its Dynamical Relaxation
- Non-canonical statistics of finite quantum system
- Quantum dynamics of the intramolecular vibrational energy redistribution in OCS: From localization to quasi-thermalization
- Typical, finite baths as a means of exact simulation of open quantum systems
- Quantum Thermodynamics, Entropy of the Universe, Free Energy, and the Second Law
Cited by in corpus (5)
- Open quantum system dynamics and the mean force Gibbs state
- Cooperative isentropic charging of hybrid quantum batteries
- Lasting effects of static magnetic field on classical Brownian motion
- Asymmetric temperature equilibration with heat flow from cold to hot in a quantum thermodynamic system
- Quantum harmonic oscillators and thermalization