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      Scaling Green-Kubo relation and application to three aging systems

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          Abstract

          The Green-Kubo formula relates the spatial diffusion coefficient to the stationary velocity autocorrelation function. We derive a generalization of the Green-Kubo formula valid for systems with long-range or nonstationary correlations for which the standard approach is no longer valid. For the systems under consideration, the velocity autocorrelation function \(\langle v(t+\tau) v(t) \rangle\) asymptotically exhibits a certain scaling behavior and the diffusion is anomalous \(\langle x^2(t) \rangle \simeq 2 D_\nu t^{\nu}\). We show how both the anomalous diffusion coefficient \(D_\nu\) and exponent \(\nu\) can be extracted from this scaling form. Our scaling Green-Kubo relation thus extends an important relation between transport properties and correlation functions to generic systems with scale invariant dynamics. This includes stationary systems with slowly decaying power law correlations as well as aging systems, whose properties depend on the the age of the system. Even for systems that are stationary in the long time limit, we find that the long time diffusive behavior can strongly depend on the initial preparation of the system. In these cases, the diffusivity \(D_{\nu}\) is not unique and we determine its values for a stationary respectively nonstationary initial state. We discuss three applications of the scaling Green-Kubo relation: Free diffusion with nonlinear friction corresponding to cold atoms diffusing in optical lattices, the fractional Langevin equation with external noise recently suggested to model active transport in cells and the L\'evy walk with numerous applications, in particular blinking quantum dots. These examples underline the wide applicability of our approach, which is able to treat very different mechanisms of anomalous diffusion.

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          Most cited references35

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          Particles and fields in fluid turbulence

          The understanding of fluid turbulence has considerably progressed in recent years. The application of the methods of statistical mechanics to the description of the motion of fluid particles, i.e. to the Lagrangian dynamics, has led to a new quantitative theory of intermittency in turbulent transport. The first analytical description of anomalous scaling laws in turbulence has been obtained. The underlying physical mechanism reveals the role of statistical integrals of motion in non-equilibrium systems. For turbulent transport, the statistical conservation laws are hidden in the evolution of groups of fluid particles and arise from the competition between the expansion of a group and the change of its geometry. By breaking the scale-invariance symmetry, the statistically conserved quantities lead to the observed anomalous scaling of transported fields. Lagrangian methods also shed new light on some practical issues, such as mixing and turbulent magnetic dynamo.
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            Weak ergodicity breaking and aging in disordered systems

            J Bouchaud (1992)
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              Lévy dynamics of enhanced diffusion: Application to turbulence

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                Author and article information

                Journal
                20 October 2013
                Article
                10.1103/PhysRevX.4.011022
                1310.5405
                fdb4d735-e4c0-4e0b-b052-85bef42523f4

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

                History
                Custom metadata
                Phys. Rev. X 4, 011022 (2014)
                16 pages, 6 figures, 1 table
                cond-mat.stat-mech

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