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      How Electronic Dynamics with Pauli Exclusion Produces Fermi-Dirac Statistics

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          Abstract

          It is important that any dynamics method approaches the correct population distribution at long times. In this paper, we derive a one-body reduced density matrix dynamics for electrons in energetic contact with a bath. We obtain a remarkable equation of motion which shows that in order to reach equilibrium properly, rates of electron transitions depend on the density matrix. Even though the bath drives the electrons towards a Boltzmann distribution, hole blocking factors in our equation of motion cause the electronic populations to relax to a Fermi-Dirac distribution. These factors are an old concept, but we show how they can be derived with a combination of time-dependent perturbation theory, and the extended normal ordering of Mukherjee and Kutzelnigg. The resulting non-equilibrium kinetic equations generalize the usual Redfield theory to many-electron systems, while ensuring that the orbital occupations remain between zero and one. In numerical applications of our equations, we show that relaxation rates of molecules are not constant because of the blocking effect. Other applications to model atomic chains are also presented which highlight the importance of treating both dephasing and relaxation. Finally we show how the bath localizes the electron density matrix.

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          Normal order and extended Wick theorem for a multiconfiguration reference wave function

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            Mixed quantum-classical equilibrium: Surface hopping.

            We re-examine the analysis of the equilibrium limits of the fewest switches surface hopping algorithm for mixed quantum-classical dynamics. In contrast with previously reported results, we show that surface hopping does not, in general, exactly yield Boltzmann equilibrium, but that in practice the observed deviations are quite small. We also demonstrate that surface hopping does approach the exact equilibrium distribution in both the limits of small adiabatic splitting and/or strong nonadiabatic coupling. We verify these analytical results with numerical simulations for a simple two-level quantum system connected to a bath of classical particles.
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              Nonequilibrium steady state transport via the reduced density matrix operator

              We present a very simple model for numerically describing the steady state dynamics of a system interacting with continua of states representing a bath. Our model can be applied to equilibrium and nonequilibrium problems. For a one-state system coupled to two free electron reservoirs, our results match the Landauer formula for current traveling through a molecule. More significantly, we can also predict the nonequilibrium steady state population on a molecule between two out-of-equilibrium contacts. While the method presented here is for one-electron Hamiltonians, we outline how this model may be extended to include electron-electron interactions and correlations, an approach which suggests a connection between the conduction problem and the electronic structure problem.
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                Author and article information

                Journal
                19 November 2014
                2015-01-15
                Article
                10.1063/1.4916822
                1411.5324
                0153c29f-b46a-4b9b-ac6f-4114351a09f3

                http://creativecommons.org/licenses/by/3.0/

                History
                Custom metadata
                Revision #1: 18 pages, 4 figures. Theory sections are revised to include derivation steps
                quant-ph cond-mat.stat-mech physics.chem-ph

                Condensed matter,Quantum physics & Field theory,Physical chemistry
                Condensed matter, Quantum physics & Field theory, Physical chemistry

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