33 Coulomb FunctionsVariables ρ,η

§33.11 Asymptotic Expansions for Large ρ

For large ρ, with ℓ and η fixed,

33.11.1 Hℓ±⁡(η,ρ)∼e±i⁢θℓ⁡(η,ρ)⁢∑k=0∞(a)k⁢(b)kk!⁢(±2⁢i⁢ρ)k,

where θℓ⁡(η,ρ) is defined by (33.2.9), and a and b are defined by (33.8.3).

An equivalent formulation is given by

33.11.2 Fℓ⁡(η,ρ) =g⁡(η,ρ)⁢cos⁡θℓ+f⁡(η,ρ)⁢sin⁡θℓ,
Gℓ⁡(η,ρ) =f⁡(η,ρ)⁢cos⁡θℓ−g⁡(η,ρ)⁢sin⁡θℓ,
33.11.3 Fℓ′⁡(η,ρ) =g^⁡(η,ρ)⁢cos⁡θℓ+f^⁡(η,ρ)⁢sin⁡θℓ,
Gℓ′⁡(η,ρ) =f^⁡(η,ρ)⁢cos⁡θℓ−g^⁡(η,ρ)⁢sin⁡θℓ,
33.11.4 Hℓ±⁡(η,ρ)=e±i⁢θℓ⁢(f⁡(η,ρ)±i⁢g⁡(η,ρ)),

where

33.11.5 f⁡(η,ρ) ∼∑k=0∞fk,
g⁡(η,ρ) ∼∑k=0∞gk,
33.11.6 f^⁡(η,ρ) ∼∑k=0∞f^k,
g^⁡(η,ρ) ∼∑k=0∞g^k,
33.11.7 g⁡(η,ρ)⁢f^⁡(η,ρ)−f⁡(η,ρ)⁢g^⁡(η,ρ)=1.

Here f0=1, g0=0, f^0=0, g^0=1−(η/ρ), and for k=0,1,2,…,

33.11.8 fk+1 =λk⁢fk−μk⁢gk,
gk+1 =λk⁢gk+μk⁢fk,
f^k+1 =λk⁢f^k−μk⁢g^k−(fk+1/ρ),
g^k+1 =λk⁢g^k+μk⁢f^k−(gk+1/ρ),

where

33.11.9 λk =(2⁢k+1)⁢η(2⁢k+2)⁢ρ,
μk =ℓ⁢(ℓ+1)−k⁢(k+1)+η2(2⁢k+2)⁢ρ.