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Dunkl operator

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1: 18.38 Mathematical Applications
Dunkl Type Operators and Nonsymmetric Orthogonal Polynomials
The Dunkl operator, introduced by Dunkl (1989), is an operator associated with reflection groups or root systems which has terms involving first order partial derivatives and reflection terms. Analogues of the original Dunkl operator (the rational case) were introduced by Heckman and Cherednik for the trigonometric case, and by Cherednik for the q -case. … In the one-variable case the Dunkl operator eigenvalue equation … …
2: 37.19 Other Orthogonal Polynomials of d Variables
For 1 j d , the Dunkl operator T j is defined by …
3: 37.16 Orthogonal Polynomials on the Hyperoctant
The spaces 𝒱 n 𝜶 ( + d ) are eigenspaces of a second order partial differential operator:
37.16.4 = 1 d ( x D x 2 + ( α + 1 x ) D x ) u ( x ) = n u ( x ) , u 𝒱 n 𝜶 ( + d ) .
37.16.5 = 1 d L ν ( α ) ( x ) , ν 1 + + ν d = n .
37.16.6 Q 𝝂 , k 𝜶 ( 𝐱 ) = L n k ( 2 k + | 𝜶 | + 1 ) ( | 𝐱 | ) | 𝐱 | k P 𝝂 𝜶 ( x 1 | 𝐱 | , , x d 1 | 𝐱 | ) , 0 k n , ν 0 d 1 , | 𝝂 | = n k ,
37.16.9 lim β β k P 𝝂 β , 𝜶 ( 1 β 1 | 𝐱 | , β 1 x 1 , , β 1 x d 1 ) = Q 𝝂 , k 𝜶 ( 𝐱 ) , 𝐱 = ( x 1 , , x d ) , | 𝝂 | = n , ν 1 = n k .
4: 37.17 Hermite Polynomials on d
The spaces 𝒱 n ( d ) are eigenspaces of a second order partial differential operator, see (37.17.10). …
37.17.4 | 𝝂 | = n H 𝝂 ( 𝐱 ) 𝝂 ! 𝐲 𝝂 = 1 n ! π 1 2 H n ( 𝐱 , 𝐲 + t 1 𝐲 2 ) e t 2 d t , 𝐲 1 ,
The spaces 𝒱 n ( d ) are eigenspaces of a second order partial differential operator:
37.17.10 ( 1 2 Δ = 1 d x D x ) u ( x ) = n u ( x ) , u 𝒱 n ( d ) .
See (37.11.1) for the Laplace operator Δ . …
5: Bibliography T
  • S. Tsujimoto, L. Vinet, and A. Zhedanov (2012) Dunkl shift operators and Bannai-Ito polynomials. Adv. Math. 229 (4), pp. 2123–2158.
  • 6: 37.15 Orthogonal Polynomials on the Ball
    The spaces 𝒱 n α ( 𝔹 d ) are eigenspaces of a second order partial differential operator, see (37.15.16). …
    37.15.5 C 𝝂 ( α + 1 2 ) ( 𝐱 ) = j = 1 d ( 1 ( x 1 2 + + x j 1 2 ) ) 1 2 ν j C ν j ( α + ν j + 1 + + ν d + 1 2 ( d j + 1 ) ) ( x j 1 ( x 1 2 + + x j 1 2 ) )
    See Dunkl and Xu (2014, Proposition 5.2.2) for the explicit value of C 𝝂 ( α + 1 2 ) , C 𝝂 ( α + 1 2 ) α . … See Dunkl and Xu (2014, §5.2.2) for expressions of of these biorthogonal polynomials in terms of Lauricella’s hypergeometric function F B . … The spaces 𝒱 n α ( 𝔹 d ) are eigenspaces of a second order partial differential operator: …
    7: null
    error generating summary
    8: 37.4 Disk with Weight Function ( 1 x 2 y 2 ) α
    The spaces 𝒱 n α are eigenspaces of a second order partial differential operator, see (37.4.28). … See Dunkl and Xu (2014, §3.3.4) for multi-term relations satisfied by the OPs (37.4.5). … See Dunkl and Xu (2014, Proposition 2.3.6). … For these results see Appell and Kampé de Fériet (1926, pp. 263, 269), Erdélyi et al. (1953b, §§12.5, 12.6) (with s = 2 α + 1 ) and Dunkl and Xu (2014, §2.3) (with μ = α + 1 2 ). … The spaces 𝒱 n α of OPs on 𝔻 are eigenspaces of a second order partial differential operator: …
    9: 37.3 Triangular Region with Weight Function x α y β ( 1 x y ) γ
    The spaces 𝒱 n α , β , γ are eigenspaces of a second order partial differential operator, see (37.3.14). …
    37.3.3 P k , n α , β , γ ( x , y ) = P n k ( β + γ + 2 k + 1 , α ) ( 2 x 1 ) ( 1 x ) k P k ( γ , β ) ( 2 y 1 x 1 ) , 0 k n , α , β , γ > 1 ,
    37.3.4 P k , n α , β , γ , P j , m α , β , γ α , β , γ = h k , n α , β , γ δ n , m δ k , j , α , β , γ > 1 ,
    The coefficients in these expressions are F 3 4 hypergeometric functions that can be written in terms of Racah polynomials, see (Dunkl, 1984, Theorem 1.7) and (Iliev and Xu, 2017, Proposition 4.2). … The spaces 𝒱 n α , β , γ of OPs on are eigenspaces of a second order partial differential operator (PDO): …
    10: 18.28 Askey–Wilson Class
    In Tsujimoto et al. (2012) an extension of the Bannai–Ito polynomials occurs as eigenfunctions of a Dunkl type operator. …