With
, and
replaced by
, the modified Bessel’s equation
(10.25.1) becomes
For
and
define
Then
and
,
are real and
linearly independent solutions of (10.45.1):
As ![]()
As ![]()
where
is as in §10.24. The corresponding result for
is given by
when
, and
where
again denotes Euler’s constant (§5.2(ii)).
In consequence of (10.45.5)–(10.45.7),
and
comprise a numerically
satisfactory pair of solutions of (10.45.1) when
is large, and
either
and
, or
and
, comprise a numerically satisfactory pair when
is small, depending whether
or
.
For graphs of
and
see
§10.26(iii).