2015
DOI: 10.48550/arxiv.1510.01809
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Implicit renewal theory for exponential functionals of Lévy processes

Abstract: We establish a new functional relation for the probability density function of the exponential functional of a Lévy process, which allows to significantly simplify the techniques commonly used in the study of these random variables and hence provide quick proofs of known results, derive new results, as well as sharpening known estimates for the distribution. We apply this formula to provide another look to the Wiener-Hopf type factorisation for exponential functionals obtained in a series of papers by Pardo, P… Show more

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Cited by 5 publications
(9 citation statements)
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“…The form of the density follows from Theorem 1 of Arista and Rivero [3]. We finish our proof by observing that The asymptotic behaviour of the positive moments of Z t has been studied in Palau et al [29] using a fine study of the negative moments of exponential functional of Lévy processes.…”
Section: Population Model With Competition In a Lévy Random Environmentmentioning
confidence: 65%
See 2 more Smart Citations
“…The form of the density follows from Theorem 1 of Arista and Rivero [3]. We finish our proof by observing that The asymptotic behaviour of the positive moments of Z t has been studied in Palau et al [29] using a fine study of the negative moments of exponential functional of Lévy processes.…”
Section: Population Model With Competition In a Lévy Random Environmentmentioning
confidence: 65%
“…It is not difficult to see that Z is a weak solution to (3). In order to prove our result, we consider two solutions to (3), Z ′ and Z ′′ , and consider τ ′ p = inf{t ≥ 0 :…”
Section: Stochastic Differential Equationsmentioning
confidence: 92%
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“…Let Π − α be the Lévy measure of |α|η − . The behaviour of P − 1 (I ≤ t) as t → 0 is given in Theorem 7 of [1]. More precisely, provided that Π…”
Section: Behaviour Of the Expectationmentioning
confidence: 99%
“…(recall that η + (0) = 0 under P + 1 ). Proposition 2 in [10] gives the finiteness and an expression for the negative moments of I η + , under the assumption that e η + (1) positive moments of all order. However, the proof straightforwardly adapts to E + 1 (I…”
Section: The Upper Boundmentioning
confidence: 99%