On the properties of Laplace transform originating from one-sided Lévy stable laws

preprint2016arXivOpen access

Abstract

We consider the conventional Laplace transform of f(x)f(x), denoted by L[f(x);p] ≡ F(p)=∫0∞e−pxf(x)dx\mathcal{L}[f(x); p]~\equiv~F(p)=\int_{0}^{\infty} e^{-p x} f(x) dx with Re(p)>0{\rm \mathfrak{Re}}(p) > 0. For 0<α<10 < α< 1 we furnish the closed form expressions for the inverse Laplace transforms L−1[F(pα);x]\mathcal{L}^{-1}[F(p^α); x] and L−1[pα−1F(pα);x]\mathcal{L}^{-1}[p^{α-1}F(p^α); x]. In both cases they involve definite integration with kernels which are appropriately rescaled one-sided Lévy stable probability distribution functions gα(x)g_α(x), 0<α<10 < α< 1, x>0x > 0. Since gα(x)g_α(x) are exactly and explicitly known for rational αα, \textit{i.e.} for α=l/kα= l/k with l,k=1,2,…l, k=1, 2, \ldots, l<kl < k, our results extend the known and tabulated case of α=1/2α= 1/2 to any rational 0<α<10 < α< 1. We examine the integral kernels of this procedure as well as the resulting two kinds of Lévy integral transformations.

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