Sequences, Series, and Special Functions 641
= r( c) r1 th-1(1 - t)c-a-b-1 dt
r(b)r(c-b) } 0
=
r(c) r(b)r(c - a - b) r(c)r(c - a - b)
r(b)r(c-b) r(c-a) = r(c-a)r(c-b)
The passage to the limit under the integral sign is justified by the uniform
convergence of the integral over the integral 0 :::; x :::; 1. In fact, since
1-t:::; 1-xt:::; 1
for 0 :::; x :::; 1, 0 :::; t ::=; 1, we have
itb-1(l -w-b-1(l - xt)-al:::; tReb-1(1-t)h-1
where we let h = Re( c - b - a) > 0 if Re a > 0, and h = Re( c - b) > 0 in
the case Re a < 0. Now the B-integral
11 tRe b-1 (1 - t)h-1 dt
converges under the conditions Re( c - b - a) > 0 and Rec > Re b > 0, so,
under such conditions, the integral
11 tb-1(1 - q-b-1(1 - xt)-a dt
converges absolutely and uniformly with respect to x E (0, 1].
However, the restriction Rec > Re b > 0, which is required by the
method of proof used above, can be removed. This follows from the identity
principle for analytic functions, since both sides of the formula
r(c)r(c - a - b)
F( a, b, c; l) = r( c - a )r( c - b)
are analytic in a, b, and c, provided that c is neither zero nor a negative
integer and Re(c - a - b) > 0.
8.23 The Confluent Hypergeometric Function
Definition 8.9 The function
«I>(a, c; z) = f \a())n zn = lim F (a, b, c; ~)
n=O n. c n b-->oo
(8.23-1)
is known as the confluent hypergeometric function, or Kummer function
(also as the Pochhammer-Barnes confluent hypergeometric function). As