For the confluent hypergeometric function and the generalized hypergeometric function , the Laguerre polynomial and the Whittaker function see §16.2(ii), §16.2(iv), (18.5.12), and (13.14.3), respectively.
18.34.1 | |||
With the notation of Koekoek et al. (2010, (9.13.1)) the left-hand side of (18.34.1) has to be replaced by . Other notations in use are given by
18.34.2 | ||||
where is a modified spherical Bessel function (10.49.9), and
18.34.3 | ||||
Often only the polynomials (18.34.2) are called Bessel polynomials, while the polynomials (18.34.1) and (18.34.3) are called generalized Bessel polynomials. Sometimes the polynomials are called reverse Bessel polynomials. See also §10.49(ii).
18.34.4 | |||
where
18.34.5 | ||||
The product of coefficients in (18.34.4) is positive if and only if . Hence the full system of polynomials cannot be orthogonal on the line with respect to a positive weight function, but this is possible for a finite system of such polynomials, the Romanovski–Bessel polynomials, if :
18.34.5_5 | |||
. | |||
The full system satisfies orthogonality with respect to a (not positive definite) moment functional; see Evans et al. (1993, (2.7)) for the simple expression of the moments . Explicit (but complicated) weight functions taking both positive and negative values have been found such that (18.2.26) holds with ; see Durán (1993), Evans et al. (1993), and Maroni (1995).
Orthogonality of the full system on the unit circle can be given with a much simpler weight function:
18.34.6 | |||
, | |||
the integration path being taken in the positive rotational sense. See Ismail (2009, (4.10.9)) for orthogonality on the unit circle for general values of .
18.34.7 | |||
where primes denote derivatives with respect to . With functions
18.34.7_1 | |||
, , | |||
expressed in terms of Romanovski–Bessel polynomials, Laguerre polynomials or Whittaker functions, we have
18.34.7_2 | |||
and
18.34.7_3 | |||
. | |||
18.34.8 | |||
In this limit the finite system of Jacobi polynomials which is orthogonal on (see §18.3) tends to the finite system of Romanovski–Bessel polynomials which is orthogonal on (see (18.34.5_5)).
For uniform asymptotic expansions of as in terms of Airy functions (§9.2) see Wong and Zhang (1997) and Dunster (2001c). For uniform asymptotic expansions in terms of Hermite polynomials see López and Temme (1999b).
For further information on Bessel polynomials see §10.49(ii).