10.45 Functions of Imaginary Order10.47 Definitions and Basic Properties

§10.46 Generalized and Incomplete Bessel Functions; Mittag-Leffler Function

The function \mathop{\phi\/}\nolimits\!\left(\rho,\beta;z\right) is defined by

10.46.1 \mathop{\phi\/}\nolimits\!\left(\rho,\beta;z\right)=\sum _{{k=0}}^{\infty}\frac{z^{k}}{k!\mathop{\Gamma\/}\nolimits\!\left(\rho k+\beta\right)}, \rho>-1.

From (10.25.2)

10.46.2 \mathop{I_{{\nu}}\/}\nolimits\!\left(z\right)=\left(\tfrac{1}{2}z\right)^{\nu}\mathop{\phi\/}\nolimits\!\left(1,\nu+1;\tfrac{1}{4}z^{2}\right).

For asymptotic expansions of \mathop{\phi\/}\nolimits\!\left(\rho,\beta;z\right) as z\to\infty in various sectors of the complex z-plane for fixed real values of \rho and fixed real or complex values of \beta, see Wright (1935) when \rho>0, and Wright (1940b) when -1<\rho<0. For exponentially-improved asymptotic expansions in the same circumstances, together with smooth interpretations of the corresponding Stokes phenomenon (§§2.11(iii)2.11(v)) see Wong and Zhao (1999b) when \rho>0, and Wong and Zhao (1999a) when -1<\rho<0.

The Laplace transform of \mathop{\phi\/}\nolimits\!\left(\rho,\beta;z\right) can be expressed in terms of the Mittag-Leffler function:

10.46.3 \mathop{E_{{a,b}}\/}\nolimits\!\left(z\right)=\sum _{{k=0}}^{\infty}\frac{z^{k}}{\mathop{\Gamma\/}\nolimits\!\left(ak+b\right)}, a>0.

See Paris (2002c). This reference includes exponentially-improved asymptotic expansions for \mathop{E_{{a,b}}\/}\nolimits\!\left(z\right) when |z|\to\infty, together with a smooth interpretation of Stokes phenomena. See also Wong and Zhao (2002a), and for further information on the Mittag-Leffler function see Erdélyi et al. (1955, §18.1) and Paris and Kaminski (2001, §5.1.4).

For incomplete modified Bessel functions and Hankel functions, including applications, see Cicchetti and Faraone (2004).