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30 Spheroidal Wave FunctionsProperties

§30.11 Radial Spheroidal Wave Functions

Contents

§30.11(i) Definitions

Denote

30.11.1\psi_{k}^{{(j)}}(z)=\left(\frac{\pi}{2z}\right)^{{\frac{1}{2}}}{\cal C}_{{k+%
\frac{1}{2}}}^{{(j)}}(z),j=1,2,3,4,

where

with \mathop{J_{{\nu}}\/}\nolimits, \mathop{Y_{{\nu}}\/}\nolimits, \mathop{{H^{{(1)}}_{{\nu}}}\/}\nolimits, and \mathop{{H^{{(2)}}_{{\nu}}}\/}\nolimits as in §10.2(ii). Then solutions of (30.2.1) with \mu=m and \lambda=\mathop{\lambda^{{m}}_{{n}}\/}\nolimits\!\left(\gamma^{2}\right) are given by

30.11.3\mathop{S^{{m(j)}}_{{n}}\/}\nolimits\!\left(z,\gamma\right)=\frac{(1-z^{{-2}})%
^{{\frac{1}{2}m}}}{A_{n}^{{-m}}(\gamma^{2})}\sum_{{2k\geq m-n}}a^{{-m}}_{{n,k}%
}(\gamma^{2})\psi_{{n+2k}}^{{(j)}}(\gamma z).

Here a^{{-m}}_{{n,k}}(\gamma^{2}) is defined by (30.8.2) and (30.8.6), and

In (30.11.3) z\neq 0 when j=1, and |z|>1 when j=2,3,4.

§30.11(ii) Graphics

See accompanying text
Figure 30.11.1: \mathop{S^{{0(1)}}_{{n}}\/}\nolimits\!\left(x,2\right), n=0,1, 1\leq x\leq 10. Magnify
See accompanying text
Figure 30.11.2: \mathop{S^{{0(1)}}_{{n}}\/}\nolimits\!\left(iy,2i\right), n=0,1, 0\leq y\leq 10. Magnify
See accompanying text
Figure 30.11.3: \mathop{S^{{1(1)}}_{{n}}\/}\nolimits\!\left(x,2\right), n=1,2, 1\leq x\leq 10. Magnify
See accompanying text
Figure 30.11.4: \mathop{S^{{1(1)}}_{{n}}\/}\nolimits\!\left(iy,2i\right), n=1,2, 0\leq y\leq 10. Magnify

§30.11(iii) Asymptotic Behavior

For asymptotic expansions in negative powers of z see Meixner and Schäfke (1954, p. 293).

§30.11(v) Connection with the \mathop{\mathit{Ps}\/}\nolimits and \mathop{\mathit{Qs}\/}\nolimits Functions

§30.11(vi) Integral Representations

For further relations see Arscott (1964b, §8.6), Connett et al. (1993), Erdélyi et al. (1955, §16.13), Meixner and Schäfke (1954), and Meixner et al. (1980, §3.1).