Bessel Function of the Second Kind
A Bessel function of the second kind
(e.g, Gradshteyn
and Ryzhik 2000, p. 703, eqn. 6.649.1), sometimes also denoted
(e.g, Gradshteyn
and Ryzhik 2000, p. 657, eqn. 6.518), is a solution to the Bessel
differential equation which is singular at the origin. Bessel functions of the
second kind are also called Neumann functions or Weber functions. The above plot
shows
for
, 1, 2, ...,
5. The Bessel function of the second kind is implemented in the Wolfram
Language as BesselY[nu,
z].
Let
be the first solution and
be the other one (since the Bessel
differential equation is second-order,
there are two linearly independent
solutions). Then
|
(1)
| |||
|
(2)
|
|
(3)
|
|
(4)
|
so
, where
is a constant.
Divide by
,
|
(5)
|
|
(6)
|
Rearranging and using
gives
|
(7)
| |||
|
(8)
|
where
is the so-called Bessel function of
the second kind.
can be defined by
|
(9)
|
(Abramowitz and Stegun 1972, p. 358), where
is a Bessel function of the first kind and,
for
an integer
by the series
![]() |
(10)
|
where
is the digamma
function (Abramowitz and Stegun 1972, p. 360).
The function has the integral representations
|
(11)
| |||
![]() |
(12)
|
(Abramowitz and Stegun 1972, p. 360).
![]() |
(13)
| ||
|
(14)
|
where
is a gamma
function.

For the special case
,
is given
by the series
![]() |
(15)
|
(Abramowitz and Stegun 1972, p. 360), where
is the Euler-Mascheroni
constant and
is a harmonic
number.
^k)/(k!(n+k)!),](/National_Library/20161007105358im_/http://mathworld.wolfram.com/images/equations/BesselFunctionoftheSecondKind/NumberedEquation6.gif)

![{2/pi[ln(1/2x)+gamma] m=0,x<<1; -(Gamma(m))/pi(2/x)^m m!=0,x<<1](/National_Library/20161007105358im_/http://mathworld.wolfram.com/images/equations/BesselFunctionoftheSecondKind/Inline39.gif)
![Y_0(z)=2/pi{[ln(1/2z)+gamma]J_0(z)+sum_(k=1)^infty(-1)^(k+1)H_k((1/4z^2)^k)/((k!)^2)},](/National_Library/20161007105358im_/http://mathworld.wolfram.com/images/equations/BesselFunctionoftheSecondKind/NumberedEquation7.gif)
Anger function

