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14 Legendre and Related FunctionsReal Arguments

§14.12 Integral Representations

Contents
  1. §14.12(i) −1<x<1
  2. §14.12(ii) 1<x<∞

§14.12(i) −1<x<1

Mehler–Dirichlet Formula

14.12.1 𝖯νμ⁡(cos⁡θ) =21/2⁢(sin⁡θ)μπ1/2⁢Γ⁡(12−μ)⁢∫0θcos⁡((ν+12)⁢t)(cos⁡t−cos⁡θ)μ+(1/2)⁢dt,
0<θ<π, ℜ⁡μ<12.
14.12.2 𝖯ν−μ⁡(x) =(1−x2)−μ/2Γ⁡(μ)⁢∫x1𝖯ν⁡(t)⁢(t−x)μ−1⁢dt,
ℜ⁡μ>0;

compare (14.6.6).

14.12.3 𝖰νμ⁡(cos⁡θ)=π1/2⁢Γ⁡(ν+μ+1)⁢(sin⁡θ)μ2μ+1⁢Γ⁡(μ+12)⁢Γ⁡(ν−μ+1)×(∫0∞(sinh⁡t)2⁢μ(cos⁡θ+i⁢sin⁡θ⁢cosh⁡t)ν+μ+1⁢dt+∫0∞(sinh⁡t)2⁢μ(cos⁡θ−i⁢sin⁡θ⁢cosh⁡t)ν+μ+1⁢dt),
0<θ<π, ℜ⁡μ>−12, ℜ⁡ν±μ>−1.

§14.12(ii) 1<x<∞

14.12.4 Pν−μ⁡(x) =21/2⁢Γ⁡(μ+12)⁢(x2−1)μ/2π1/2⁢Γ⁡(ν+μ+1)⁢Γ⁡(μ−ν)⁢∫0∞cosh⁡((ν+12)⁢t)(x+cosh⁡t)μ+(1/2)⁢dt,
ν+μ≠−1,−2,−3,…, ℜ⁡(μ−ν)>0.
14.12.5 Pν−μ⁡(x) =(x2−1)−μ/2Γ⁡(μ)⁢∫1xPν⁡(t)⁢(x−t)μ−1⁢dt,
ℜ⁡μ>0.
14.12.6 𝑸νμ⁡(x) =π1/2⁢(x2−1)μ/22μ⁢Γ⁡(μ+12)⁢Γ⁡(ν−μ+1)⁢∫0∞(sinh⁡t)2⁢μ(x+(x2−1)1/2⁢cosh⁡t)ν+μ+1⁢dt,
ℜ⁡(ν+1)>ℜ⁡μ>−12.
14.12.7 Pνm⁡(x) =(ν+1)mπ⁢∫0π(x+(x2−1)1/2⁢cos⁡ϕ)ν⁢cos⁡(m⁢ϕ)⁢dϕ,
14.12.8 Pnm⁡(x) =2m⁢m!⁢(n+m)!⁢(x2−1)m/2(2⁢m)!⁢(n−m)!⁢π⁢∫0π(x+(x2−1)1/2⁢cos⁡ϕ)n−m⁢(sin⁡ϕ)2⁢m⁢dϕ,
n≥m.
14.12.9 𝑸nm⁡(x)=1n!⁢∫0u(x−(x2−1)1/2⁢cosh⁡t)n⁢cosh⁡(m⁢t)⁢dt,

where

14.12.10 u=12⁢ln⁡(x+1x−1).
14.12.11 𝑸nm⁡(x)=(x2−1)m/22n+1⁢n!⁢∫−11(1−t2)n(x−t)n+m+1⁢dt,

Neumann’s Integral

14.12.13 𝑸n⁡(x)=12⁢(n!)⁢∫−11Pn⁡(t)x−t⁢dt.

Heine’s Integral

For further integral representations see Erdélyi et al. (1953a, pp. 158–159) and Magnus et al. (1966, pp. 184–190), and for contour integrals and other representations see §14.25.