Abstract

The generalized Langevin equation is a model for the motion of coarse-grained particles where dissipative forces are represented by a memory term. The numerical realization of such a model requires the implementation of a stochastic delay-differential equation and the estimation of a corresponding memory kernel. Here we develop a new approach for computing a data-driven Markov model for the motion of the particles, given equidistant samples of their velocity autocorrelation function. Our method bypasses the determination of the underlying memory kernel by representing it via up to about twenty auxiliary variables. The algorithm is based on a sophisticated variant of the Prony method for exponential interpolation and employs the positive real lemma from model reduction theory to extract the associated Markov model. We demonstrate the potential of this approach for the test case of anomalous diffusion, where data are given analytically, and then apply our method to velocity autocorrelation data of molecular dynamics simulations of a colloid in a Lennard-Jones fluid. In both cases, the velocity autocorrelation function and the memory kernel can be reproduced very accurately. Moreover, we show that the algorithm can also handle input data with large statistical noise. We anticipate that it will be a very useful tool in future studies that involve dynamic coarse-graining of complex soft matter systems.

Highlights

  • Generalized Langevin Equations (GLE)s, i.e., extensions of Langevin equations with memory, have fascinated scientists for many decades, ever since they were first introduced by Mori in the 60s [40] based on concepts of Zwanzig [52]

  • We have addressed the problem of mapping GLEs onto equivalent extended Markovian Langevin equations which can be integrated more in numerical simulations

  • We have developed an analytical method to extract the parameters of the extended Markovian system directly from the knowledge of the autocorrelation function of the target quantity, without knowledge of the memory kernel in the GLE

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Summary

Introduction

Generalized Langevin Equations (GLE)s, i.e., extensions of Langevin equations with memory, have fascinated scientists for many decades, ever since they were first introduced by Mori in the 60s [40] based on concepts of Zwanzig [52] Their purpose is to describe in very general terms the irreversible dynamics of collective (coarse-grained) observables in many-particle systems without having to assume complete separation of time scales. Consider a multiparticle system at thermal equilibrium, and assume we are interested in the dynamical evolution of a given set A(t) of coarse-grained variables For such cases, starting from a microscopic Hamiltonian description and using a projection operator formalism, Mori and Zwanzig derived a dynamical equation of the following form for A(t) [53] t.

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