[go: up one dir, main page]

18 Orthogonal PolynomialsClassical Orthogonal Polynomials

§18.11 Relations to Other Functions

Contents
  1. §18.11(i) Explicit Formulas
  2. §18.11(ii) Formulas of Mehler–Heine Type

§18.11(i) Explicit Formulas

See §§18.5(i) and 18.5(iii) for relations to trigonometric functions, the hypergeometric function, and generalized hypergeometric functions.

Ultraspherical

18.11.1 𝖯nm⁡(x)=(12)m⁢(−2)m⁢(1−x2)12⁢m⁢Cn−m(m+12)⁡(x)=(n+1)m⁢(−2)−m⁢(1−x2)12⁢m⁢Pn−m(m,m)⁡(x),
0≤m≤n.

For the Ferrers function 𝖯nm⁡(x), see §14.3(i).

Compare also (14.3.21) and (14.3.22).

Laguerre

For the confluent hypergeometric functions M⁡(a,b,x) and U⁡(a,b,x), see §13.2(i), and for the Whittaker functions Mκ,μ⁡(x) and Wκ,μ⁡(x) see §13.14(i).

Hermite

18.11.3 Hn⁡(x) =2n⁢U⁡(−12⁢n,12,x2)=2n⁢x⁢U⁡(−12⁢n+12,32,x2)=212⁢n⁢e12⁢x2⁢U⁡(−n−12,212⁢x),
18.11.4 𝐻𝑒n⁡(x) =212⁢n⁢U⁡(−12⁢n,12,12⁢x2)=212⁢(n−1)⁢x⁢U⁡(−12⁢n+12,32,12⁢x2)=e14⁢x2⁢U⁡(−n−12,x).

For the parabolic cylinder function U⁡(a,z), see §12.2.

§18.11(ii) Formulas of Mehler–Heine Type

Jacobi

18.11.5 limn→∞1nα⁢Pn(α,β)⁡(1−z22⁢n2)=limn→∞1nα⁢Pn(α,β)⁡(cos⁡zn)=2αzα⁢Jα⁡(z).

Laguerre

18.11.6 limn→∞1nα⁢Ln(α)⁡(zn)=1z12⁢α⁢Jα⁡(2⁢z12).

Hermite

18.11.7 limn→∞(−1)n⁢n1222⁢n⁢n!⁢H2⁢n⁡(z2⁢n12) =1π12⁢cos⁡z,
18.11.8 limn→∞(−1)n22⁢n⁢n!⁢H2⁢n+1⁡(z2⁢n12) =2π12⁢sin⁡z.

For the Bessel function Jν⁡(z), see §10.2(ii). The limits (18.11.5)–(18.11.8) hold uniformly for z in any bounded subset of ℂ.