2006
DOI: 10.1007/s00220-005-1492-5
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Mott Law as Lower Bound for a Random Walk in a Random Environment

Abstract: We consider a random walk on the support of an ergodic stationary simple point process on R d , d ≥ 2, which satisfies a mixing condition w.r.t. the translations or has a strictly positive density uniformly on large enough cubes. Furthermore the point process is furnished with independent random bounded energy marks. The transition rates of the random walk decay exponentially in the jump distances and depend on the energies through a factor of the Boltzmann-type. This is an effective model for the phonon-induc… Show more

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Cited by 29 publications
(115 citation statements)
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References 27 publications
(21 reference statements)
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“…The above bound is in agreement with Mott law (1.6). We note that the requirement α > 0 in [8][Theorem 1] is due to a typing error. Moreover it is simple to check that, although in [8] the transition rates c x,y (ξ) are defined as in (1.4), all the results in [8] remain true for transition rates c x,y (ξ) defined as in (1.7) and assuming only that α > −1.…”
Section: Model and Resultsmentioning
confidence: 99%
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“…The above bound is in agreement with Mott law (1.6). We note that the requirement α > 0 in [8][Theorem 1] is due to a typing error. Moreover it is simple to check that, although in [8] the transition rates c x,y (ξ) are defined as in (1.4), all the results in [8] remain true for transition rates c x,y (ξ) defined as in (1.7) and assuming only that α > −1.…”
Section: Model and Resultsmentioning
confidence: 99%
“…The analogous of Mott law (1.3) for Mott variable-range random walk is given by 6) where D(β) denotes the diffusion matrix of the random walk. For dimension d ≥ 2, a lower bound of D(β) in agreement with (1.6) has been recently proven in [8]. The present work addresses to the problem of rigorously deriving an upper bound of D(β) in agreement with (1.6).…”
mentioning
confidence: 78%
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“…[1][2][3][4][5][6][7][8][9][10][11] As shown already by Mott,12 this mobility can be understood to result from thermally assisted variable-range hopping ͑VRH͒ between localized states of varying energy. Mott thereby considers a single-hop rate of the form exp͑−␣R − ␤͒ ͑␣ is the inverse localization length and ␤ =1/k B T͒ first introduced by Miller and Abrahams, 13 which accounts both for tunneling through the tail of the wave function and for a phonon-assisted thermal activation.…”
Section: Introductionmentioning
confidence: 98%