2020
DOI: 10.30757/alea.v17-01
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A weak overdamped limit theorem for Langevin processes

Abstract: In this paper, we prove convergence in distribution of Langevin processes in the overdamped asymptotics. The proof relies on the classical perturbed test function (or corrector) method, which is used both to show tightness in path space, and to identify the extracted limit with a martingale problem. The result holds assuming the continuity of the gradient of the potential energy, and a mild control of the initial kinetic energy.Date: December 1, 2018. 1991

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Cited by 3 publications
(5 citation statements)
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“…Our results are complementary to those in [19] in the following sense: First, there the authors have to assume the interaction term ∇Φ 1 to be continuous. Second, there the state space is assumed to be the d−dimensional torus T d .…”
Section: Introductionmentioning
confidence: 47%
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“…Our results are complementary to those in [19] in the following sense: First, there the authors have to assume the interaction term ∇Φ 1 to be continuous. Second, there the state space is assumed to be the d−dimensional torus T d .…”
Section: Introductionmentioning
confidence: 47%
“…the invariant measure µ Φ . This aspect is more restrictive than in [19]. Additionally, the Φ 1 in [19] may also depend on ε > 0.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…which is more precise than (26). It suffices to combine (28) and Assumption 2 to obtain (26). Observe that if p 0 " 0, the strong error estimate (28) yields the following refinement of ( 26 where the error estimate is uniform with respect to both the time-scale separation parameter P p0, 0 q and to the temporal index n P t0, .…”
Section: 3mentioning
confidence: 99%
“…The convergence result q Ñ q 0 is often called a Smoluchowski-Kramers diffusion approximation result in the literature. If σ is constant and equal to the identity, and if f " ´∇V for some potential energy function V : R d Ñ R, the SDE system (1) describes the Langevin dynamics, whereas the SDE (2) describes the overdamped Langevin dynamics, see for instance [17,Section 6.3.4], [19, Sections 2.2.3 and 2.2.4], [23,Section 6.5], and also the recent article [26] and references therein. We also refer to the monographs [17], [19] and [23] for analysis and applications of (overdamped) Langevin dynamics.…”
Section: Charles-edouard Br éHiermentioning
confidence: 99%