2018
DOI: 10.1214/18-ejp202
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Bernstein-gamma functions and exponential functionals of Lévy processes

Abstract: In this work we analyse the solution to the recurrence equationMΨ(z), MΨ(1) = 1, defined on a subset of the imaginary line and where −Ψ runs through the set of all continuous negative definite functions. Using the analytic Wiener-Hopf method we furnish the solution to this equation as a product of functions that extend the classical gamma function. These latter functions, being in bijection with the class of Bernstein functions, are called Bernsteingamma functions. Using their Weierstrass product representatio… Show more

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Cited by 63 publications
(151 citation statements)
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References 64 publications
(142 reference statements)
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“…Let f (x) = e −x which is strictly decreasing on R. Then since (−∞, 0) is P-transient and ∞ 0 e −y U (dy) is finite being the U 1 potential, we conclude that the following ∞ 0 e −ξs ds < ∞ holds. This elementary fact is well-known from the theory of exponential functionals of Lévy processes, see Patie, P. and Savov, M. (2018), but illustrates the applicability of our result. We also emphasize that from Lemma 4.6 and the proof of the main theorem for relation (2.4) to hold it suffices to know that the set…”
Section: Notation and Main Resultssupporting
confidence: 80%
“…Let f (x) = e −x which is strictly decreasing on R. Then since (−∞, 0) is P-transient and ∞ 0 e −y U (dy) is finite being the U 1 potential, we conclude that the following ∞ 0 e −ξs ds < ∞ holds. This elementary fact is well-known from the theory of exponential functionals of Lévy processes, see Patie, P. and Savov, M. (2018), but illustrates the applicability of our result. We also emphasize that from Lemma 4.6 and the proof of the main theorem for relation (2.4) to hold it suffices to know that the set…”
Section: Notation and Main Resultssupporting
confidence: 80%
“…In order to avoid the trivial situation when T = ∞ P x -almost surely (a.s.), according to Lamperti, see also [25,Section 2.2], it suffices that…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The sufficient conditions for N = ∞ are easily derived. The fact that ϑ + α (dy) = v + α (y)dy, y > 0, with v + α (0 + ) ∈ (0, ∞) follows from [25,Proposition B.2]. Next, from (2.6), we get that for all t > 0,…”
Section: End Of the Proof Of Theorem 11mentioning
confidence: 88%
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