2019
DOI: 10.1007/978-3-030-15096-9_8
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Ergodic Properties of Quasi-Markovian Generalized Langevin Equations with Configuration Dependent Noise and Non-conservative Force

Abstract: We discuss the ergodic properties of quasi-Markovian stochastic differential equations, providing general conditions that ensure existence and uniqueness of a smooth invariant distribution and exponential convergence of the evolution operator in suitably weighted L ∞ spaces, which implies the validity of central limit theorem for the respective solution processes. The main new result is an ergodicity condition for the generalized Langevin equation with configuration-dependent noise and (non-)conservative force. Show more

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Cited by 12 publications
(12 citation statements)
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References 61 publications
(178 reference statements)
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“…The matrices Γ M and Σ are such that the operator ∂ t − L GLE is hypoelliptic. (see [28,Proposition 7] for sufficient algebraic conditions on Γ M , Σ for Hypoellipticity of the operator.) In particular,…”
Section: Assumptionmentioning
confidence: 99%
See 1 more Smart Citation
“…The matrices Γ M and Σ are such that the operator ∂ t − L GLE is hypoelliptic. (see [28,Proposition 7] for sufficient algebraic conditions on Γ M , Σ for Hypoellipticity of the operator.) In particular,…”
Section: Assumptionmentioning
confidence: 99%
“…Under the above stated assumptions exponential convergence of the associated semi-group and a central limit theorem for trajectory averages can be established: Proposition 1.2 ( [28]). Let Assumptions 1 to 3 be satisfied.…”
Section: Assumptionmentioning
confidence: 99%
“…The success of the hypoellipticity method inspires us to develop a hypocoercivity theory for analyzing the dynamical behavior of the EMZ equation. The hypocoercivity method was mainly developed by Villani [40], Dolbeault, Mouhot and Schmeiser [4] and many other researchers [12,13,11,20,19] to study the kinetic equations in a pure functional analysis framework. For detailed explorations in this regard, we refer to the above papers and the reference therein.…”
Section: Introductionmentioning
confidence: 99%
“…The last term η(t) is the noise which is the fluctuation part of the interaction between the system and the heat bath. Later, the GLE was recovered by dimension reduction from Ford-Kac and Kac-Zwanzig models using Mori-Zwanzig projection ( [16,17,18,19]). In the GLE models, the noise η and the kernel for the friction γ(·) satisfy the so-called fluctuation-dissipation theorem (FDT) E(η(t)η(t + τ )) = kT γ(|τ |), ∀τ ∈ R.…”
Section: Introductionmentioning
confidence: 99%