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18 Orthogonal PolynomialsClassical Orthogonal Polynomials

§18.10 Integral Representations

Contents
  1. §18.10(i) Dirichlet–Mehler-Type Integral Representations
  2. §18.10(ii) Laplace-Type Integral Representations
  3. §18.10(iii) Contour Integral Representations
  4. §18.10(iv) Other Integral Representations

§18.10(i) Dirichlet–Mehler-Type Integral Representations

Ultraspherical

18.10.1 Pn(α,α)⁡(cos⁡θ)Pn(α,α)⁡(1)=Cn(α+12)⁡(cos⁡θ)Cn(α+12)⁡(1)=2α+12⁢Γ⁡(α+1)π12⁢Γ⁡(α+12)⁢(sin⁡θ)−2⁢α⁢∫0θcos⁡((n+α+12)⁢ϕ)(cos⁡ϕ−cos⁡θ)−α+12⁢dϕ,
0<θ<π, α>−12.

Legendre

18.10.2 Pn⁡(cos⁡θ)=212π⁢∫0θcos⁡((n+12)⁢ϕ)(cos⁡ϕ−cos⁡θ)12⁢dϕ,
0<θ<π.

Generalizations of (18.10.1) for Pn(α,β) are given in Gasper (1975, (6),(8)) and Koornwinder (1975a, (5.7),(5.8)).

§18.10(ii) Laplace-Type Integral Representations

Jacobi

18.10.3 Pn(α,β)⁡(cos⁡θ)Pn(α,β)⁡(1)=2⁢Γ⁡(α+1)π12⁢Γ⁡(α−β)⁢Γ⁡(β+12)⁢∫01∫0π((cos⁡12⁢θ)2−r2⁢(sin⁡12⁢θ)2+i⁢r⁢sin⁡θ⁢cos⁡ϕ)n×(1−r2)α−β−1⁢r2⁢β+1⁢(sin⁡ϕ)2⁢β⁢dϕ⁢dr,
α>β>−12.

Ultraspherical

18.10.4 Pn(α,α)⁡(cos⁡θ)Pn(α,α)⁡(1)=Cn(α+12)⁡(cos⁡θ)Cn(α+12)⁡(1)=Γ⁡(α+1)π12⁢Γ⁡(α+12)⁢∫0π(cos⁡θ+i⁢sin⁡θ⁢cos⁡ϕ)n⁢(sin⁡ϕ)2⁢α⁢dϕ,
α>−12.

Legendre

18.10.5 Pn⁡(cos⁡θ)=1π⁢∫0π(cos⁡θ+i⁢sin⁡θ⁢cos⁡ϕ)n⁢dϕ.

Laguerre

18.10.6 Ln(α)⁡(x2)=2⁢(−1)nπ12⁢Γ⁡(α+12)⁢n!⁢∫0∞∫0π(x2−r2+2⁢i⁢x⁢r⁢cos⁡ϕ)n⁢e−r2×r2⁢α+1⁢(sin⁡ϕ)2⁢α⁢dϕ⁢dr,
α>−12.

Hermite

§18.10(iii) Contour Integral Representations

Table 18.10.1 gives contour integral representations of the form

18.10.8 pn⁡(x)=g0⁡(x)2⁢π⁢i⁢∫C(g1⁡(z,x))n⁢g2⁡(z,x)⁢(z−c)−1⁢dz

for the Jacobi, Laguerre, and Hermite polynomials. Here C is a simple closed contour encircling z=c once in the positive sense.

Table 18.10.1: Classical OP’s: contour integral representations (18.10.8).
pn⁡(x) g0⁡(x) g1⁡(z,x) g2⁡(z,x) c Conditions
Pn(α,β)⁡(x) (1−x)−α⁢(1+x)−β z2−12⁢(z−x) (1−z)α⁢(1+z)β x ±1 outside C.
Cn(λ)⁡(x) 1 z−1 (1−2⁢x⁢z+z2)−λ 0 e±i⁢θ outside C (where x=cos⁡θ).
Tn⁡(x) 1 z−1 1−x⁢z1−2⁢x⁢z+z2 0
Un⁡(x) 1 z−1 (1−2⁢x⁢z+z2)−1 0
Pn⁡(x) 1 z−1 (1−2⁢x⁢z+z2)−12 0
Pn⁡(x) 1 z2−12⁢(z−x) 1 x
Ln(α)⁡(x) ex⁢x−α z⁢(z−x)−1 zα⁢e−z x 0 outside C.
Hn⁡(x)/n! 1 z−1 e2⁢x⁢z−z2 0
𝐻𝑒n⁡(x)/n! 1 z−1 ex⁢z−12⁢z2 0

§18.10(iv) Other Integral Representations

Laguerre

18.10.9 Ln(α)⁡(x)=ex⁢x−12⁢αn!⁢∫0∞e−t⁢tn+12⁢α⁢Jα⁡(2⁢x⁢t)⁢dt,
α>−1.

For the Bessel function Jν⁡(z) see §10.2(ii).

Hermite

18.10.10 Hn⁡(x)=(−2⁢i)n⁢ex2π12⁢∫−∞∞e−t2⁢tn⁢e2⁢i⁢x⁢t⁢dt=2n+1π12⁢ex2⁢∫0∞e−t2⁢tn⁢cos⁡(2⁢x⁢t−12⁢n⁢π)⁢dt.

See also §18.17.