30 Spheroidal Wave FunctionsProperties

§30.5 Functions of the Second Kind

Other solutions of (30.2.1) with μ=m, λ=λnm⁡(γ2), and z=x are

30.5.1 𝖰𝗌nm⁡(x,γ2),
n=m,m+1,m+2,….

They satisfy

30.5.2 𝖰𝗌nm⁡(−x,γ2)=(−1)n−m+1⁢𝖰𝗌nm⁡(x,γ2),

and

compare §14.3(i). Also,

30.5.4 𝒲⁡{𝖯𝗌nm⁡(x,γ2),𝖰𝗌nm⁡(x,γ2)}=(n+m)!(1−x2)⁢(n−m)!⁢Anm⁡(γ2)⁢An−m⁡(γ2)(≠0),

with An±m⁡(γ2) as in (30.11.4).

For further properties see Meixner and Schäfke (1954) and §30.8(ii).