2014
DOI: 10.1016/j.spa.2013.11.003
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Unavoidable collections of balls for isotropic Lévy processes

Abstract: A collection tBpx n , r n qu ně1 of pairwise disjoint balls in the Euclidean space R d is said to be avoidable with respect to a transient process X if the process with positive probability escapes to infinity without hitting any ball. In this paper we study sufficient and necessary conditions for avoidability with respect to unimodal isotropic Lévy processes satisfying a certain scaling hypothesis. These conditions are expressed in terms of the characteristic exponent of the process, or alternatively, in term… Show more

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Cited by 10 publications
(14 citation statements)
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References 20 publications
(49 reference statements)
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“…Our first three results provide estimates of the probability of hitting a ball, the potential kernel and the Green function of a ball. All of them improve previously known results: for hitting probabilities, see Lemma 2.5 in [33], Proposition 5.8 in [5] and Lemmas 3.4 2010 Mathematics Subject Classification. Primary: 60J35, 60J50; secondary: 60J75, 31B25.…”
Section: Introductionsupporting
confidence: 83%
“…Our first three results provide estimates of the probability of hitting a ball, the potential kernel and the Green function of a ball. All of them improve previously known results: for hitting probabilities, see Lemma 2.5 in [33], Proposition 5.8 in [5] and Lemmas 3.4 2010 Mathematics Subject Classification. Primary: 60J35, 60J50; secondary: 60J75, 31B25.…”
Section: Introductionsupporting
confidence: 83%
“…For the Brownian semigroup (classical potential theory) and isotropic αstable semigroups (Riesz potentials) we have g(r) = r α−d , α ∈ (0, 2], α < d, and our assumptions are satisfied with R 0 = R 1 = 0. This holds as well for the more general isotropic unimodal Lévy semigroups considered in [11].…”
supporting
confidence: 60%
“…In the more general case of isotropic unimodal Lévy processes, where the characteristic function satisfies a lower scaling condition (and (LD), (UD) hold with R 0 = R 1 = 0), both Theorem 1.2, its converse, and Corollary 1.3 are proven in [11]. We shall use the same method of considering finitely many countable unions of concentric shells, but have to overcome additional difficulties caused by having only a rather weak estimate for the exit distribution of balls (compare [11,Lemma 2.2], going back to [5,Corollary 2], and Proposition 3.7). Nevertheless our proof for Theorem 1.2 can be simpler, since starting with an avoidable union A and an arbitrary δ > 0, we may assume without loss of generality that P 0 [T A < ∞] < δ (using Proposition 3.3 and translation invariance).…”
mentioning
confidence: 97%
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