Finite quantum environments as thermostats: an analysis based on the Hilbert space average method
arXiv:quant-ph/0612062 · doi:10.1140/epjb/e2006-00407-3
Abstract
We consider discrete quantum systems coupled to finite environments which may possibly consist of only one particle in contrast to the standard baths which usually consist of continua of oscillators, spins, etc. We find that such finite environments may, nevertheless, act as thermostats, i.e., equilibrate the system though not necessarily in the way predicted by standard open system techniques. Thus, we apply a novel technique called the Hilbert space Average Method (HAM) and verify its results numerically.
12 pages, 10 figures
References in corpus (8)
- Concepts and methods in the theory of open quantum systems
- Canonical Typicality
- Decoherence, Chaos, and the Second Law
- Thermalizing Quantum Machines: Dissipation and Entanglement
- Non-Markovian quantum dynamics: Correlated projection superoperators and Hilbert space averaging
- Quantum Approach to a Derivation of the Second Law of Thermodynamics
- Thermalization of quantum systems by finite baths
- From Pure Schroedingerian to Statistical Dynamics
Cited by in corpus (17)
- Finite-size scaling of eigenstate thermalization
- Adding dynamical generators in quantum master equations
- Occurrence of exponential relaxation in closed quantum systems
- Classicality, Markovianity and local detailed balance from pure state dynamics
- Origin of the Canonical Ensemble: Thermalization with Decoherence
- Approach to equilbrium in nano-scale systems at finite temperatur
- The approach to typicality in many-body quantum systems
- Quantum Decoherence Scaling with Bath Size: Importance of Dynamics, Connectivity, and Randomness
- Monogamy and backflow of mutual information in non-Markovian thermal baths
- Quantum Heat Baths satisfying the eigenstate thermalization hypothesis
- Fermi's golden rule, the origin and breakdown of Markovian master equations, and the relationship between oscillator baths and the random matrix model
- Steepest Entropy Ascent for Two-State Systems with Slowly Varying Hamiltonians
- Typical, finite baths as a means of exact simulation of open quantum systems
- Boltzmann equation approach to transport in finite modular quantum systems
- Effective environments: Preparation of stationary states with inverse temperature ranging from positive to negative values
- Perturbative treatment for stationary state of local master equation
- Interplay of decoherence and relaxation in a two-level system interacting with an infinite-temperature reservoir