2009
DOI: 10.1214/ecp.v14-1497
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From the Lifshitz tail to the quenched survival asymptotics in the trapping problem

Abstract: The survival problem for a diffusing particle moving among random traps is considered. We introduce a simple argument to derive the quenched asymptotics of the survival probability from the Lifshitz tail effect for the associated operator. In particular, the upper bound is proved in fairly general settings and is shown to be sharp in the case of the Brownian motion in the Poissonian obstacles. As an application, we derive the quenched asymptotics for the Brownian motion in traps distributed according to a rand… Show more

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Cited by 12 publications
(16 citation statements)
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“…The localization problem in the quenched case was far more challenging: in the Brownian setting it was studied first in [29,32] and its logarithmic asymptotics for the survival probability was first derived in [29] (see also the celebrated monograph [33]). In [12] a simple argument for the quenched asymptotics of the survival probability was given using the Lifshitz tail effect. In the random walk setting, the logarithmic asymptotics of survival probability was computed in [1] which built upon methods developed in the Brownian setting.…”
Section: University Of Pennsylvania and University Of Chicagomentioning
confidence: 99%
“…The localization problem in the quenched case was far more challenging: in the Brownian setting it was studied first in [29,32] and its logarithmic asymptotics for the survival probability was first derived in [29] (see also the celebrated monograph [33]). In [12] a simple argument for the quenched asymptotics of the survival probability was given using the Lifshitz tail effect. In the random walk setting, the logarithmic asymptotics of survival probability was computed in [1] which built upon methods developed in the Brownian setting.…”
Section: University Of Pennsylvania and University Of Chicagomentioning
confidence: 99%
“…where λ BM 1 (B(0, 1)) is the principal eigenvalue for the Brownian motion killed on exiting B(0, 1). This result was reproven by Fukushima [9]. For the Brownian motion on some irregular spaces such as the Sierpiński gasket, one also sees a similar phenomenon: rates of the annealed and the quenched asymptotics differ (see [28,29]).…”
Section: 2)mentioning
confidence: 79%
“…To the best of our knowledge the quenched asymptotics for Lévy processes with jumps has not been studied before. In the literature concerning the Brownian motion, one finds two methods: Sznitman's paper [34] estimates u ω (t, x) directly, using his 'enlargement of obstacles' technique for the more difficult upper bound (similar method was used on the Sierpiński gasket in [28]); Fukushima [9] gives elegant arguments for deriving both the upper and the lower quenched bound from respective upper and lower bounds at zero for the integrated density of states of the corresponding Schrödinger operator (being closely related to the annealed upper and lower bounds) -this is done by means of the Dirichlet-Neumann bracketing for the Laplace operator. In our work, we are able to find a counterpart of Fukushima's method for Lévy processes with jumps to obtain the upper bounds.…”
Section: 2)mentioning
confidence: 99%
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“…This connection was utilized in [Fuk09b] for deriving relations between asymptotics of .E/ for E # inf . …”
Section: Integrated Density Of Statesmentioning
confidence: 99%