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18 Orthogonal PolynomialsClassical Orthogonal Polynomials

§18.7 Interrelations and Limit Relations

Contents
  1. §18.7(i) Linear Transformations
  2. §18.7(ii) Quadratic Transformations
  3. §18.7(iii) Limit Relations

§18.7(i) Linear Transformations

Ultraspherical and Jacobi

18.7.1 Cn(λ)⁡(x) =(2⁢λ)n(λ+12)n⁢Pn(λ−12,λ−12)⁡(x),
18.7.2 Pn(α,α)⁡(x) =(α+1)n(2⁢α+1)n⁢Cn(α+12)⁡(x).

Chebyshev, Ultraspherical, and Jacobi

18.7.3 Tn⁡(x)=Pn(−12,−12)⁡(x)/Pn(−12,−12)⁡(1),
18.7.4 Un⁡(x)=Cn(1)⁡(x)=(n+1)⁢Pn(12,12)⁡(x)/Pn(12,12)⁡(1),
18.7.5 Vn⁡(x)=Pn(−12,12)⁡(x)/Pn(−12,12)⁡(1),
18.7.6 Wn⁡(x)=(2⁢n+1)⁢Pn(12,−12)⁡(x)/Pn(12,−12)⁡(1).
18.7.7 Tn∗⁡(x) =Tn⁡(2⁢x−1),
18.7.8 Un∗⁡(x) =Un⁡(2⁢x−1).

See also (18.9.9)–(18.9.12). For (18.7.3) see also (18.7.25).

Legendre, Ultraspherical, and Jacobi

18.7.9 Pn⁡(x)=Cn(12)⁡(x)=Pn(0,0)⁡(x).
18.7.10 Pn∗⁡(x)=Pn⁡(2⁢x−1).

Hermite

18.7.11 𝐻𝑒n⁡(x) =2−12⁢n⁢Hn⁡(2−12⁢x),
18.7.12 Hn⁡(x) =212⁢n⁢𝐻𝑒n⁡(212⁢x).

§18.7(ii) Quadratic Transformations

18.7.13 P2⁢n(α,α)⁡(x)P2⁢n(α,α)⁡(1) =Pn(α,−12)⁡(2⁢x2−1)Pn(α,−12)⁡(1),
18.7.14 P2⁢n+1(α,α)⁡(x)P2⁢n+1(α,α)⁡(1) =x⁢Pn(α,12)⁡(2⁢x2−1)Pn(α,12)⁡(1).
18.7.15 C2⁢n(λ)⁡(x) =(λ)n(12)n⁢Pn(λ−12,−12)⁡(2⁢x2−1),
18.7.16 C2⁢n+1(λ)⁡(x) =(λ)n+1(12)n+1⁢x⁢Pn(λ−12,12)⁡(2⁢x2−1).
18.7.17 U2⁢n⁡(x) =Wn⁡(2⁢x2−1),
18.7.18 T2⁢n+1⁡(x) =x⁢Vn⁡(2⁢x2−1).
18.7.19 H2⁢n⁡(x) =(−1)n⁢22⁢n⁢n!⁢Ln(−12)⁡(x2),
18.7.20 H2⁢n+1⁡(x) =(−1)n⁢22⁢n+1⁢n!⁢x⁢Ln(12)⁡(x2).

Equations (18.7.13)–(18.7.20) are special cases of (18.2.22)–(18.2.23).

§18.7(iii) Limit Relations

Jacobi → Laguerre

18.7.21 limβ→∞Pn(α,β)⁡(1−(2⁢x/β))=Ln(α)⁡(x).
18.7.22 limα→∞Pn(α,β)⁡((2⁢x/α)−1)=(−1)n⁢Ln(β)⁡(x).

Jacobi → Hermite

18.7.23 limα→∞α−12⁢n⁢Pn(α,α)⁡(α−12⁢x)=Hn⁡(x)2n⁢n!.

Ultraspherical → Hermite

18.7.24 limλ→∞λ−12⁢n⁢Cn(λ)⁡(λ−12⁢x)=Hn⁡(x)n!.

Ultraspherical → Chebyshev

18.7.25 limλ→0n+λλ⁢Cn(λ)⁡(x)={1,n=0,2⁢Tn⁡(x),n=1,2,….

Laguerre → Hermite

18.7.26 limα→∞(2α)12⁢n⁢Ln(α)⁡((2⁢α)12⁢x+α)=(−1)nn!⁢Hn⁡(x).

See Figure 18.21.1 for the Askey schematic representation of most of these limits. See §18.11(ii) for limit formulas of Mehler–Heine type.