2012
DOI: 10.1239/jap/1331216836
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A Fourier Approach for the Level Crossings of Shot Noise Processes with Jumps

Abstract: We use a change-of-variable formula in the framework of functions of bounded variation to derive an explicit formula for the Fourier transform of the level crossing function of shot noise processes with jumps. We illustrate the result in some examples and give some applications. In particular, it allows us to study the asymptotic behavior of the mean number of level crossings as the intensity of the Poisson point process of the shot noise process goes to infinity.

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Cited by 12 publications
(10 citation statements)
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“…More generally, the theory presented here can be seen as a reference model for intermittent fluctuations and is well known to be relevant for many other applications beyond fusion plasmas. 48,49,56,57 …”
Section: Discussionmentioning
confidence: 99%
“…More generally, the theory presented here can be seen as a reference model for intermittent fluctuations and is well known to be relevant for many other applications beyond fusion plasmas. 48,49,56,57 …”
Section: Discussionmentioning
confidence: 99%
“…The books [2] and [6] contain a comprehensive update of these subjects. Crossings for discontinuous processes have been considered in [10], [15] and [16], the two last works include KRFs. The shot noise process has received attention in regard to crossing problems and KRF (see Biermé & Desolneux, [11] and [13]).…”
Section: Introductionmentioning
confidence: 99%
“…We start from a particular case of the results derived in Ref. 5 for the Fourier amplitude of the level crossing functionN X (u): the case of piecewise, nonincreasing pulse-shapes g(t) with an arbitrary number of finite jumps (such functions satisfẏ g(t) ≤ 0 inside each interval between two jumps),…”
Section: A Derivation Of the Level Crossing Rate N X (U )mentioning
confidence: 99%
“…(20) reduces to a generalization of the experimentally well established paralyzable pile-up model. 5 The pulse-height spectrum then reduces to p(U) = δ(U −U 0 ), U 0 being the pulseheight corresponding to the energy E 0 with the final result (A = 0):…”
Section: A Derivation Of the Level Crossing Rate N X (U )mentioning
confidence: 99%