2016
DOI: 10.1016/j.spa.2015.10.007
|View full text |Cite
|
Sign up to set email alerts
|

Einstein relation for reversible random walks in random environment on Z

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

1
8
0

Year Published

2017
2017
2019
2019

Publication Types

Select...
2
1

Relationship

0
3

Authors

Journals

citations
Cited by 3 publications
(9 citation statements)
references
References 9 publications
1
8
0
Order By: Relevance
“…negative) half-line and that it is not differentiable at λ = 0. For this model we also prove the Einstein Relation, both in discrete and continuous time, extending the result of [25].…”
supporting
confidence: 71%
See 3 more Smart Citations
“…negative) half-line and that it is not differentiable at λ = 0. For this model we also prove the Einstein Relation, both in discrete and continuous time, extending the result of [25].…”
supporting
confidence: 71%
“…We prove the Einstein relation under two different sets of assumptions: the first one requires the ergodicity of the conductances and some moments conditions; we point out that this is the equivalent set of conditions that [25] would require in our setting, but we give an alternative, shorter proof. We extend this result including a different hypothesis, just requiring the weakest possible integrability of the conductances and very mild mixing conditions.…”
Section: Einstein Relationmentioning
confidence: 99%
See 2 more Smart Citations
“…A weaker form of the Einstein relation, which is often used as a starting point, was proved in [29]. Since then, the analysis of the Einstein relation, the steady states and the linear response for random walks in static/dynamic random environments have been addressed in [2,3,17,18,19,23,24,27,28,30,31,33,35] (the list is not exhaustive). The approach used here is different from the previous works: Although the distribution Q λ is not explicit, by refining the analysis of [12] we prove that the Radon-Nikodym derivative dQ λ dQ 0 belongs to L p (Q 0 ) if E e pZ 0 < ∞ for some p ≥ 2 (see Theorem 1).…”
Section: Introductionmentioning
confidence: 99%