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16 Generalized Hypergeometric Functions & Meijer G-FunctionGeneralized Hypergeometric Functions

§16.8 Differential Equations

Contents
  1. §16.8(i) Classification of Singularities
  2. §16.8(ii) The Generalized Hypergeometric Differential Equation
  3. §16.8(iii) Confluence of Singularities

§16.8(i) Classification of Singularities

An ordinary point of the differential equation

16.8.1 \frac{{\mathrm{d}}^{n}w}{{\mathrm{d}z}^{n}}+f_{n-1}(z)\frac{{\mathrm{d}}^{n-1}%
w}{{\mathrm{d}z}^{n-1}}+f_{n-2}(z)\frac{{\mathrm{d}}^{n-2}w}{{\mathrm{d}z}^{n-%
2}}+\dots+f_{1}(z)\frac{\mathrm{d}w}{\mathrm{d}z}+f_{0}(z)w=0

is a value z_{0} of z at which all the coefficients f_{j}(z), j=0,1,\dots,n-1, are analytic. If z_{0} is not an ordinary point but (z-z_{0})^{n-j}f_{j}(z), j=0,1,\dots,n-1, are analytic at z=z_{0}, then z_{0} is a regular singularity. All other singularities are irregular. Compare §2.7(i) in the case n=2. Similar definitions apply in the case z_{0}=\infty: we transform \infty into the origin by replacing z in (16.8.1) by 1/z; again compare §2.7(i).

For further information see Hille (1976, pp. 360–370).

§16.8(ii) The Generalized Hypergeometric Differential Equation

With the notation

16.8.2
D=\frac{\mathrm{d}}{\mathrm{d}z},
\vartheta=z\frac{\mathrm{d}}{\mathrm{d}z},

the function w={{}_{p}F_{q}}\left(\mathbf{a};\mathbf{b};z\right) satisfies the differential equation

Equivalently,

or

where \alpha_{j} and \beta_{j} are constants. Equation (16.8.4) has a regular singularity at z=0, and an irregular singularity at z=\infty, whereas (16.8.5) has regular singularities at z=0, 1, and \infty. In each case there are no other singularities. Equation (16.8.3) is of order \max(p,q+1). In Letessier et al. (1994) examples are discussed in which the generalized hypergeometric function satisfies a differential equation that is of order 1 or even 2 less than might be expected.

When no b_{j} is an integer, and no two b_{j} differ by an integer, a fundamental set of solutions of (16.8.3) is given by

where * indicates that the entry 1+b_{j}-b_{j} is omitted. For other values of the b_{j}, series solutions in powers of z (possibly involving also \ln z) can be constructed via a limiting process; compare §2.7(i) in the case of second-order differential equations. For details see Smith (1939a, b), and Nørlund (1955).

When p=q+1, and no two a_{j} differ by an integer, another fundamental set of solutions of (16.8.3) is given by

where * indicates that the entry 1-a_{j}+a_{j} is omitted. We have the connection formula

More generally if z_{0} (\in\mathbb{C}) is an arbitrary constant, |z-z_{0}|>\max{(|z_{0}|,|z_{0}-1|)}, and |\operatorname{ph}\left(z_{0}-z\right)|<\pi, then

(Note that the generalized hypergeometric functions on the right-hand side are polynomials in z_{0}.)

When p=q+1 and some of the a_{j} differ by an integer a limiting process can again be applied. For details see Nørlund (1955). In this reference it is also explained that in general when q>1 no simple representations in terms of generalized hypergeometric functions are available for the fundamental solutions near z=1. Analytical continuation formulas for {{}_{q+1}F_{q}}\left(\mathbf{a};\mathbf{b};z\right) near z=1 are given in Bühring (1987b) for the case q=2, and in Bühring (1992) for the general case.

§16.8(iii) Confluence of Singularities

If p\leq q, then

Thus in the case p=q the regular singularities of the function on the left-hand side at \alpha and \infty coalesce into an irregular singularity at \infty.

Next, if p\leq q+1 and |\operatorname{ph}\beta|\leq\pi-\delta (<\pi), then

provided that in the case p=q+1 we have |z|<1 when |\operatorname{ph}\beta|\leq\frac{1}{2}\pi, and |z|<|\sin\left(\operatorname{ph}\beta\right)| when \frac{1}{2}\pi\leq|\operatorname{ph}\beta|\leq\pi-\delta (<\pi).