§16.8 Differential Equations
Contents
- §16.8(i) Classification of Singularities
- §16.8(ii) The Generalized Hypergeometric Differential Equation
- §16.8(iii) Confluence of Singularities
§16.8(i) Classification of Singularities
An ordinary point of the differential equation
is a value
of
at which all the coefficients
,
, are analytic. If
is not an ordinary point but
,
, are analytic at
, then
is a regular singularity. All other singularities are
irregular. Compare §2.7(i) in the case
. Similar
definitions apply in the case
: we transform
into the
origin by replacing
in (16.8.1) by
; 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
the function
satisfies the
differential equation
Equivalently,

or

where
and
are constants. Equation (16.8.4)
has a regular singularity at
, and an irregular singularity at
, whereas (16.8.5) has regular singularities at
, 1, and
. In each case there are no other singularities.
Equation (16.8.3) is of order
. 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
is an integer, and no two
differ by an integer, a
fundamental set of solutions of (16.8.3) is given by
where
indicates that the entry
is omitted. For other values
of the
, series solutions in powers of
(possibly involving also
) 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
, and no two
differ by an integer, another fundamental set
of solutions of (16.8.3) is given by
where
indicates that the entry
is omitted. We have the
connection formula

More
generally if
(
) is an arbitrary constant,
, and
, then
(Note that the generalized hypergeometric functions on the right-hand side are
polynomials in
.)
When
and some of the
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
no simple
representations in terms of generalized hypergeometric functions are available
for the fundamental solutions near
. Analytical continuation formulas
for
near
are given in
Bühring (1987b) for the case
, and in
Bühring (1992) for the general case.
§16.8(iii) Confluence of Singularities
If
, then
Thus in the case
the regular singularities of the function on the
left-hand side at
and
coalesce into an irregular singularity
at
.
Next, if
and
(
), then
provided that in the case
we have
when
, and
when
(
).

