Quantum weak invariants: Dynamical evolution of fluctuations and correlations
arXiv:2009.07959 · doi:10.3390/e22111219
Abstract
Weak invariants are time-dependent observables with conserved expectation values. Their fluctuations, however, do not remain constant in time. On the assumption that time evolution of the state of an open quantum system is given in terms of a completely positive map, the fluctuations monotonically grow even if the map is not unital, in contrast to the fact that monotonic increases of both the von Neumann entropy and Rényi entropy require the map to be unital. In this way, the weak invariants describe temporal asymmetry in a manner different from the entropies. A formula is presented for time evolution of the covariance matrix associated with the weak invariants in the case when the system density matrix obeys the Gorini-Kossakowski-Lindblad-Sudarshan equation.
arXiv comment21 pages, no figures
References in corpus (13)
- Black Hole Entropy is Noether Charge
- A Brief History of the GKLS Equation
- Lindbladian operators, von Neumann entropy and energy conservation in time-dependent quantum open systems
- Time evolution of Renyi entropy under the Lindblad equation
- Weak invariants of time-dependent quantum dissipative systems
- Classical states via decoherence
- A general treatment of geometric phases and dynamical invariants
- The direction of time and Boltzmann's time hypothesis
- Weak invariants, temporally-local equilibria, and isoenergetic processes described by the Lindblad equation
- Selection of Squeezed States via Decoherence
- Action principle and weak invariants
- Weak invariants in dissipative systems: Action principle and Noether charge for kinetic theory
- Growing fluctuation of quantum weak invariant and dissipation