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On the distribution of Brownian areas. (English) Zbl 0870.60035

Summary: We study the distributions of the areas under the positive parts of a Brownian motion process \(B\) and a Brownian bridge process \(U\): with \(A^+=\int^1_0B^+(t)dt\) and \(A^+_0= \int^1_0U^+(t)dt\), we use excursion theory to show that the Laplace transforms \(\Psi^+(s)= E\exp(-sA^+)\) and \(\Psi^+_0(s)= E\exp(-sA^+_0)\) of \(A^+\) and \(A^+_0\) satisfy \[ \int^\infty_0 e^{-\lambda s}\Psi^+(\sqrt 2s^{3/2})ds= {\lambda^{-1/2}Ai(\lambda)+ (1/3-\int^\lambda_0A_i(t)dt)\over \sqrt\lambda Ai(\lambda)-Ai'(\lambda)} \] and \[ \int^\infty_0 {e^{-\lambda s}\over\sqrt s} \Psi^+_0(\sqrt 2 s^{3/2})ds= 2\sqrt\pi {Ai(\lambda)\over\sqrt\lambda Ai(\lambda)- Ai'(\lambda)}, \] where \(Ai\) is Airy’s function. At the same time, our approach via excursion theory unifies previous calculations of this type due to Kac, Groeneboom, Louchard, Shepp and Takács for other Brownian areas. Similarly, we use excursion theory to obtain recursion formulas for the moments of the “positive part” areas. We have not yet succeeded in inverting the double Laplace transforms because of the structure of the function appearing in the denominators, namely, \(\sqrt\lambda Ai(\lambda)- Ai'(\lambda)\).

MSC:

60G15 Gaussian processes
60G99 Stochastic processes
60E05 Probability distributions: general theory
Full Text: DOI

References:

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[36] INSTITUTE FOR MATHEMATICS, physiCS UNIVERSITY OF WASHINGTON AND MECHANICS DEPARTMENT OF STATISTICS DEPARTMENT OF MATHEMATICS BOX 354322
[37] UNIVERSITY OF LJUBLJANA SEATTLE, WASHINGTON 98195-4322 JADRANSKA 19 E-MAIL: jaw@stat.washington.edu 61111 LJUBLJANA SLOVENIA E-MAIL: Mihael.Perman@fmf.uni-lj.si
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