Irreversible processes without energy dissipation in an isolated Lipkin-Meshkov-Glick model
arXiv:1404.6146 · doi:10.1103/PhysRevE.92.012101
Abstract
For a certain class of isolated quantum systems, we report the existence of irreversible processes in which the energy is not dissipated. After a closed cycle in which the initial energy distribution is fully recovered, the expectation value of a symmetry-breaking observable changes from a value different from zero in the initial state, to zero in the final state. This entails the unavoidable loss of a certain amount of information, and constitutes a source of irreversibility. We show that the von Neumann entropy of time-averaged equilibrium states increases in the same magnitude as a consequence of the process. We support this result by means of numerical calculations in an experimentally feasible system, the Lipkin-Meshkov-Glick model.
10 pages, 7 figures
References in corpus (13)
- Thermalization and its mechanism for generic isolated quantum systems
- Nonlinear atom interferometer surpasses classical precision limit
- The Physics of Maxwell's demon and information
- Entanglement in a second order quantum phase transition
- Finite-Size Scaling Exponents of the Lipkin-Meshkov-Glick Model
- Exact spectrum of the Lipkin-Meshkov-Glick model in the thermodynamic limit and finite-size corrections
- Work measurement as a generalized quantum measurement
- Second-law-like inequalities with information and their interpretations
- Adiabatic quantum dynamics of the Lipkin-Meshkov-Glick model
- Microcanonical quantum fluctuation theorems
- Excited-state phase transition leading to symmetry-breaking steady states in the Dicke model
- Microscopic expression for the heat in the adiabatic basis
- Non-thermal quantum phase transitions
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