33 Coulomb FunctionsVariables r,ϵ

§33.19 Power-Series Expansions in r

33.19.1 f(ϵ,;r)=r+1k=0αkrk,

where

33.19.2 α0 =2+1/(2+1)!,
α1 =α0/(+1),
k(k+2+1)αk+2αk1+ϵαk2=0,
k=2,3,.
33.19.3 2πh(ϵ,;r)=k=02(2k)!γkk!(2r)kk=0δkrk++1A(ϵ,)(2ln|2r/κ|+ψ(+1+κ)+ψ(+κ))f(ϵ,;r),
r0.

Here κ is defined by (33.14.6), A(ϵ,) is defined by (33.14.11) or (33.14.12), γ0=1, γ1=1, and

33.19.4 γkγk1+14(k1)(k22)ϵγk2=0,
k=2,3,.

Also,

33.19.5 δ0 =(β2+12(ψ(2+2)+ψ(1))A(ϵ,))α0,
δ1 =(β2+22(ψ(2+3)+ψ(2))A(ϵ,))α1,
33.19.6 k(k+2+1)δk+2δk1+ϵδk2+2(2k+2+1)A(ϵ,)αk=0,
k=2,3,,

with β0=β1=0, and

33.19.7 βkβk1+14(k1)(k22)ϵβk2+12(k1)ϵγk2=0,
k=2,3,.

The expansions (33.19.1) and (33.19.3) converge for all finite values of r, except r=0 in the case of (33.19.3).