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18 Orthogonal PolynomialsAskey Scheme

§18.22 Hahn Class: Recurrence Relations and Differences

Contents
  1. §18.22(i) Recurrence Relations in n
  2. §18.22(ii) Difference Equations in x
  3. §18.22(iii) x-Differences

§18.22(i) Recurrence Relations in n

Hahn

With

18.22.1 pn⁡(x)=Qn⁡(x;α,β,N),
18.22.2 −x⁢pn⁡(x)=An⁢pn+1⁡(x)−(An+Cn)⁢pn⁡(x)+Cn⁢pn−1⁡(x),

where

18.22.3 An =(n+α+β+1)⁢(n+α+1)⁢(N−n)(2⁢n+α+β+1)⁢(2⁢n+α+β+2),
Cn =n⁢(n+α+β+N+1)⁢(n+β)(2⁢n+α+β)⁢(2⁢n+α+β+1).

Krawtchouk, Meixner, and Charlier

These polynomials satisfy (18.22.2) with pn⁡(x), An, and Cn as in Table 18.22.1.

Table 18.22.1: Recurrence relations (18.22.2) for Krawtchouk, Meixner, and Charlier polynomials.
pn⁡(x) An Cn
Kn⁡(x;p,N) p⁢(N−n) n⁢(1−p)
Mn⁡(x;β,c) c⁢(n+β)1−c n1−c
Cn⁡(x;a) a n

Continuous Hahn

With

18.22.4 qn⁡(x)=pn⁡(x;a,b,a¯,b¯)/pn⁡(i⁢a;a,b,a¯,b¯),
18.22.5 (a+i⁢x)⁢qn⁡(x)=A~n⁢qn+1⁡(x)−(A~n+C~n)⁢qn⁡(x)+C~n⁢qn−1⁡(x),

where

18.22.6 A~n =−(n+2⁢ℜ⁡(a+b)−1)⁢(n+a+a¯)⁢(n+a+b¯)(2⁢n+2⁢ℜ⁡(a+b)−1)⁢(2⁢n+2⁢ℜ⁡(a+b)),
C~n =n⁢(n+b+a¯−1)⁢(n+b+b¯−1)(2⁢n+2⁢ℜ⁡(a+b)−2)⁢(2⁢n+2⁢ℜ⁡(a+b)−1).

Meixner–Pollaczek

With

18.22.7 pn⁡(x)=Pn(λ)⁡(x;ϕ),
18.22.8 (n+1)⁢pn+1⁡(x)=2⁢(x⁢sin⁡ϕ+(n+λ)⁢cos⁡ϕ)⁢pn⁡(x)−(n+2⁢λ−1)⁢pn−1⁡(x).

§18.22(ii) Difference Equations in x

Hahn

With

18.22.9 pn⁡(x)=Qn⁡(x;α,β,N),
18.22.10 A⁡(x)⁢pn⁡(x+1)−(A⁡(x)+C⁡(x))⁢pn⁡(x)+C⁡(x)⁢pn⁡(x−1)−n⁢(n+α+β+1)⁢pn⁡(x)=0,

where

18.22.11 A⁡(x) =(x+α+1)⁢(x−N),
C⁡(x) =x⁢(x−β−N−1).

Krawtchouk, Meixner, and Charlier

18.22.12 A⁡(x)⁢pn⁡(x+1)−(A⁡(x)+C⁡(x))⁢pn⁡(x)+C⁡(x)⁢pn⁡(x−1)+λn⁢pn⁡(x)=0.

For A⁡(x), C⁡(x), and λn in (18.22.12) see Table 18.22.2.

Table 18.22.2: Difference equations (18.22.12) for Krawtchouk, Meixner, and Charlier polynomials.
pn⁡(x) A⁡(x) C⁡(x) λn
Kn⁡(x;p,N) p⁢(x−N) (p−1)⁢x −n
Mn⁡(x;β,c) c⁢(x+β) x n⁢(1−c)
Cn⁡(x;a) a x n

Continuous Hahn

With

18.22.14 A⁡(x)⁢pn⁡(x+i)−(A⁡(x)+C⁡(x))⁢pn⁡(x)+C⁡(x)⁢pn⁡(x−i)+n⁢(n+2⁢ℜ⁡(a+b)−1)⁢pn⁡(x)=0,

where

18.22.15 A⁡(x) =(x+i⁢a¯)⁢(x+i⁢b¯),
C⁡(x) =(x−i⁢a)⁢(x−i⁢b).

Meixner–Pollaczek

With

18.22.16 pn⁡(x)=Pn(λ)⁡(x;ϕ),
18.22.17 A⁡(x)⁢pn⁡(x+i)−(A⁡(x)+C⁡(x))⁢pn⁡(x)+C⁡(x)⁢pn⁡(x−i)+2⁢n⁢sin⁡ϕ⁢pn⁡(x)=0,

where

18.22.18 A⁡(x) =ei⁢ϕ⁢(x+i⁢λ),
C⁡(x) =e−i⁢ϕ⁢(x−i⁢λ).

§18.22(iii) x-Differences

Hahn

18.22.19 Δx⁡Qn⁡(x;α,β,N) =−n⁢(n+α+β+1)(α+1)⁢N⁢Qn−1⁡(x;α+1,β+1,N−1),
18.22.20 ∇x((α+1)x⁢(β+1)N−xx!⁢(N−x)!⁢Qn⁡(x;α,β,N)) =N+1β⁢(α)x⁢(β)N+1−xx!⁢(N+1−x)!⁢Qn+1⁡(x;α−1,β−1,N+1).

Krawtchouk

18.22.21 Δx⁡Kn⁡(x;p,N) =−np⁢N⁢Kn−1⁡(x;p,N−1),
18.22.22 ∇x((Nx)⁢px⁢(1−p)N−x⁢Kn⁡(x;p,N)) =(N+1x)⁢px⁢(1−p)N−x⁢Kn+1⁡(x;p,N+1).

Meixner

18.22.23 Δx⁡Mn⁡(x;β,c)=−n⁢(1−c)β⁢c⁢Mn−1⁡(x;β+1,c),
18.22.24 ∇x((β)x⁢cxx!⁢Mn⁡(x;β,c))=(β−1)x⁢cxx!⁢Mn+1⁡(x;β−1,c).

Charlier

18.22.25 Δx⁡Cn⁡(x;a) =−na⁢Cn−1⁡(x;a),
18.22.26 ∇x(axx!⁢Cn⁡(x;a)) =axx!⁢Cn+1⁡(x;a).

Continuous Hahn

18.22.27 δx⁡(pn⁡(x;a,b,a¯,b¯))=(n+2⁢ℜ⁡(a+b)−1)⁢pn−1⁡(x;a+12,b+12,a¯+12,b¯+12),
18.22.28 δx⁡(w⁡(x;a+12,b+12,a¯+12,b¯+12)⁢pn⁡(x;a+12,b+12,a¯+12,b¯+12))=−(n+1)⁢w⁡(x;a,b,a¯,b¯)⁢pn+1⁡(x;a,b,a¯,b¯).

Meixner–Pollaczek

18.22.29 δx⁡(Pn(λ)⁡(x;ϕ))=2⁢sin⁡ϕ⁢Pn−1(λ+12)⁡(x;ϕ),
18.22.30 δx⁡(w(λ+12)⁡(x;ϕ)⁢Pn(λ+12)⁡(x;ϕ))=−(n+1)⁢w(λ)⁡(x;ϕ)⁢Pn+1(λ)⁡(x;ϕ).