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      Optimal transport and von Neumann entropy in an Heisenberg XXZ chain out of equilibrium

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          Abstract

          In this paper we investigate the spin currents and the von Neumann entropy (VNE) of an Heisenberg XXZ chain in contact with twisted XY-boundary magnetic reservoirs by means of the Lindblad master equation. Exact solutions for the stationary reduced density matrix are explicitly constructed for chains of small sizes by using a quantum symmetry operation of the system. These solutions are then used to investigate the optimal transport in the chain in terms of the VNE. As a result we show that the maximal spin current always occurs in the proximity of extrema of the VNE and for particular choices of parameters (coupling with reservoirs and anisotropy) it can exactly coincide with them. In the limit of strong coupling we show that minima of the VNE tend to zero, meaning that the maximal transport is achieved in this case with states that are very close to pure states.

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          The Quantum Jump Approach to Dissipative Dynamics in Quantum Optics

          Dissipation, the irreversible loss of energy and coherence, from a microsystem, is the result of coupling to a much larger macrosystem (or reservoir) which is so large that one has no chance of keeping track of all of its degrees of freedom. The microsystem evolution is then described by tracing over the reservoir states, resulting in an irreversible decay as excitation leaks out of the initially excited microsystems into the outer reservoir environment. Earlier treatments of this dissipation described an ensemble of microsystems using density matrices, either in Schroedinger picture with Master equations, or in Heisenberg picture with Langevin equations. The development of experimental techniques to study single quantum systems (for example single trapped ions, or cavity radiation field modes) has stimulated the construction of theoretical methods to describe individual realizations conditioned on a particular observation record of the decay channel, in the environment. These methods, variously described as Quantum Jump, Monte Carlo Wavefunction and Quantum Trajectory methods are the subject of this review article. We discuss their derivation, apply them to a number of current problems in quantum optics and relate them to ensemble descriptions.
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            Quantum Nonequilibrium Steady States Induced by Repeated Interactions

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              PT-Symmetric Wave Chaos

              , , (2010)
              We study a new class of chaotic systems with dynamical localization, where gain or loss mechanisms break the Hermiticity, while allowing for parity-time (PT) symmetry. For a value \gamma_PT of the gain or loss parameter the spectrum undergoes a spontaneous phase transition from real (exact phase) to complex values (broken phase). We develop a one parameter scaling theory for \gamma_PT, and show that chaos assists the exact PT phase. Our results have applications to the design of optical elements with PT symmetry.
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                Author and article information

                Journal
                10 December 2012
                Article
                10.1103/PhysRevE.87.022108
                1212.2095
                371bfff8-97c7-434d-964c-4c691d1c9870

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                8 pages, 7 figures
                cond-mat.stat-mech quant-ph

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