Confluent Hypergeometric Function of the Second Kind

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The confluent hypergeometric function of the second kind gives the second linearly independent solution to the confluent hypergeometric differential equation. It is also known as the Kummer's function of the second kind, Tricomi function, or Gordon function. It is denoted U(a,b,z) and can be defined by

U(a,b,z)=picsc(pib)[(_1F^~_1(a;b;z))/(Gamma(a-b+1))-(z^(1-b)_1F^~_1(a-b+1;2-b;z))/(Gamma(a))]
(1)
=z^(-a)_2F_0(a,1+a-b;;-z^(-1)),
(2)

where _1F^~_1(a;b;z) is a regularized confluent hypergeometric function of the first kind, Gamma(z) is a gamma function, and _2F_0(a,b;;z) is a generalized hypergeometric function (which converges nowhere but exists as a formal power series; Abramowitz and Stegun 1972, p. 504).

It has an integral representation

 U(a,b,z)=1/(Gamma(a))int_0^inftye^(-zt)t^(a-1)(1+t)^(b-a-1)dt
(3)

for R[a],R[z]>0 (Abramowitz and Stegun 1972, p. 505).

The confluent hypergeometric function of the second kind is implemented in the Wolfram Language as HypergeometricU[a, b, z].

The Whittaker functions give an alternative form of the solution.

The function has a Maclaurin series

 U(a,b,z)=-((b+az)Gamma(-b))/(Gamma(1+a-b))+(z^(1-b)Gamma(b-1))/(Gamma(a))+...,
(4)

and asymptotic series

 U(a,b,z)∼(1/z)^a[1+a(b-a-1)z^(-1) 
 +1/2a(a+1)(a+b-1)(2+b-a)z^(-2)+...].
(5)

U(a,b,z) has derivative

 d/(dz)U(a,b,z)=-aU(a+1,b+1,z)
(6)

and indefinite integral

 intU(a,b,z)dz=(G_(2,3)^(2,2)(x|1,2-a; 1,2-b,0))/(Gamma(a)Gamma(a-b+1))+C,
(7)

where G_(p,q)^(m,n)(x|a_1,...,a_p; b_1,...,b_q) is a Meijer G-function and C is a constant of integration.

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