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14 Legendre and Related FunctionsReal Arguments

§14.3 Definitions and Hypergeometric Representations

Contents
  1. §14.3(i) Interval −1<x<1
  2. §14.3(ii) Interval 1<x<∞
  3. §14.3(iii) Alternative Hypergeometric Representations
  4. §14.3(iv) Relations to Other Functions

§14.3(i) Interval −1<x<1

The following are real-valued solutions of (14.2.2) when μ, ν∈ℝ and x∈(−1,1).

Ferrers Function of the First Kind

14.3.1 𝖯νμ⁡(x)=(1+x1−x)μ/2⁢𝐅⁡(ν+1,−ν;1−μ;12−12⁢x).

Ferrers Function of the Second Kind

14.3.2 𝖰νμ⁡(x)=π2⁢sin⁡(μ⁢π)⁢(cos⁡(μ⁢π)⁢(1+x1−x)μ/2⁢𝐅⁡(ν+1,−ν;1−μ;12−12⁢x)−Γ⁡(ν+μ+1)Γ⁡(ν−μ+1)⁢(1−x1+x)μ/2⁢𝐅⁡(ν+1,−ν;1+μ;12−12⁢x)).

Here and elsewhere in this chapter

is Olver’s hypergeometric function (§15.1).

𝖯νμ⁡(x) exists for all values of μ and ν. 𝖰νμ⁡(x) is undefined when μ+ν=−1,−2,−3,….

When μ=m=0,1,2,…, (14.3.1) reduces to

14.3.4 𝖯νm⁡(x)=(−1)m⁢Γ⁡(ν+m+1)2m⁢Γ⁡(ν−m+1)⁢(1−x2)m/2⁢𝐅⁡(ν+m+1,m−ν;m+1;12−12⁢x);

equivalently,

14.3.5 𝖯νm⁡(x)=(−1)m⁢Γ⁡(ν+m+1)Γ⁡(ν−m+1)⁢(1−x1+x)m/2⁢𝐅⁡(ν+1,−ν;m+1;12−12⁢x).

When μ=m (∈ℤ) (14.3.2) is replaced by its limiting value; see Hobson (1931, §132) for details. See also (14.3.12)–(14.3.14) for this case.

§14.3(ii) Interval 1<x<∞

The following are solutions of (14.2.2) when μ, ν∈ℝ and x>1.

Associated Legendre Function of the First Kind

Associated Legendre Function of the Second Kind

14.3.7 Qνμ⁡(x)=eμ⁢π⁢i⁢π1/2⁢Γ⁡(ν+μ+1)⁢(x2−1)μ/22ν+1⁢xν+μ+1⁢𝐅⁡(12⁢ν+12⁢μ+1,12⁢ν+12⁢μ+12;ν+32;1x2),
μ+ν≠−1,−2,−3,….

When μ=m=1,2,3,…, (14.3.6) reduces to

14.3.8 Pνm⁡(x)=Γ⁡(ν+m+1)2m⁢Γ⁡(ν−m+1)⁢(x2−1)m/2⁢𝐅⁡(ν+m+1,m−ν;m+1;12−12⁢x).

As standard solutions of (14.2.2) we take the pair Pν−μ⁡(x) and 𝑸νμ⁡(x), where

and

Like Pνμ⁡(x), but unlike Qνμ⁡(x), 𝑸νμ⁡(x) is real-valued when ν, μ∈ℝ and x∈(1,∞), and is defined for all values of ν and μ. The notation 𝑸νμ⁡(x) is due to Olver (1997b, pp. 170 and 178).

§14.3(iii) Alternative Hypergeometric Representations

14.3.11 𝖯νμ⁡(x) =cos⁡(12⁢(ν+μ)⁢π)⁢w1⁡(ν,μ,x)+sin⁡(12⁢(ν+μ)⁢π)⁢w2⁡(ν,μ,x),
14.3.12 𝖰νμ⁡(x) =−12⁢π⁢sin⁡(12⁢(ν+μ)⁢π)⁢w1⁡(ν,μ,x)+12⁢π⁢cos⁡(12⁢(ν+μ)⁢π)⁢w2⁡(ν,μ,x),

where

14.3.13 w1⁡(ν,μ,x) =2μ⁢Γ⁡(12⁢ν+12⁢μ+12)Γ⁡(12⁢ν−12⁢μ+1)⁢(1−x2)−μ/2⁢𝐅⁡(−12⁢ν−12⁢μ,12⁢ν−12⁢μ+12;12;x2),
14.3.14 w2⁡(ν,μ,x) =2μ⁢Γ⁡(12⁢ν+12⁢μ+1)Γ⁡(12⁢ν−12⁢μ+12)⁢x⁢(1−x2)−μ/2⁢𝐅⁡(12−12⁢ν−12⁢μ,12⁢ν−12⁢μ+1;32;x2).
14.3.15 Pν−μ⁡(x)=2−μ⁢(x2−1)μ/2⁢𝐅⁡(μ−ν,ν+μ+1;μ+1;12−12⁢x),
14.3.16 cos⁡(ν⁢π)⁢Pν−μ⁡(x)=2ν⁢π1/2⁢xν−μ⁢(x2−1)μ/2Γ⁡(ν+μ+1)⁢𝐅⁡(12⁢μ−12⁢ν,12⁢μ−12⁢ν+12;12−ν;1x2)−π1/2⁢(x2−1)μ/22ν+1⁢Γ⁡(μ−ν)⁢xν+μ+1⁢𝐅⁡(12⁢ν+12⁢μ+1,12⁢ν+12⁢μ+12;ν+32;1x2),
14.3.17 Pν−μ⁡(x)=π⁢(x2−1)μ/22μ⁢(𝐅⁡(12⁢μ−12⁢ν,12⁢ν+12⁢μ+12;12;x2)Γ⁡(12⁢μ−12⁢ν+12)⁢Γ⁡(12⁢ν+12⁢μ+1)−x⁢𝐅⁡(12⁢μ−12⁢ν+12,12⁢ν+12⁢μ+1;32;x2)Γ⁡(12⁢μ−12⁢ν)⁢Γ⁡(12⁢ν+12⁢μ+12)),
14.3.18 Pν−μ⁡(x) =2−μ⁢xν−μ⁢(x2−1)μ/2⁢𝐅⁡(12⁢μ−12⁢ν,12⁢μ−12⁢ν+12;μ+1;1−1x2),
14.3.19 𝑸νμ⁡(x) =2ν⁢Γ⁡(ν+1)⁢(x+1)μ/2(x−1)(μ/2)+ν+1⁢𝐅⁡(ν+1,ν+μ+1;2⁢ν+2;21−x),
14.3.20 2⁢sin⁡(μ⁢π)π⁢𝑸νμ⁡(x)=(x+1)μ/2Γ⁡(ν+μ+1)⁢(x−1)μ/2⁢𝐅⁡(ν+1,−ν;1−μ;12−12⁢x)−(x−1)μ/2Γ⁡(ν−μ+1)⁢(x+1)μ/2⁢𝐅⁡(ν+1,−ν;μ+1;12−12⁢x).

For further hypergeometric representations of Pνμ⁡(x) and Qνμ⁡(x) see Erdélyi et al. (1953a, pp. 123–139), Andrews et al. (1999, §3.1), Magnus et al. (1966, pp. 153–163), and §15.8(iii). For further hypergeometric representations of 𝖰νμ⁡(x) see Cohl et al. (2021).

§14.3(iv) Relations to Other Functions

In terms of the Gegenbauer function Cα(β)⁡(x) and the Jacobi function ϕλ(α,β)⁡(t) (§§15.9(iii), 15.9(ii)):

14.3.21 𝖯νμ⁡(x) =2μ⁢Γ⁡(1−2⁢μ)⁢Γ⁡(ν+μ+1)Γ⁡(ν−μ+1)⁢Γ⁡(1−μ)⁢(1−x2)μ/2⁢Cν+μ(12−μ)⁡(x).
14.3.22 Pνμ⁡(x) =2μ⁢Γ⁡(1−2⁢μ)⁢Γ⁡(ν+μ+1)Γ⁡(ν−μ+1)⁢Γ⁡(1−μ)⁢(x2−1)μ/2⁢Cν+μ(12−μ)⁡(x).
14.3.23 Pνμ⁡(x) =1Γ⁡(1−μ)⁢(x+1x−1)μ/2⁢ϕ−i⁢(2⁢ν+1)(−μ,μ)⁡(arcsinh⁡((12⁢x−12)1/2)).

Compare also (18.11.1). From (15.9.15) it follows that 1−2⁢μ=0,−1,−2,… and ν+μ+1=0,−1,−2,… are removable singularities of the right-hand sides of (14.3.21) and (14.3.22).