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discrete q-Hermite I and II polynomials

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11: 18.25 Wilson Class: Definitions
§18.25 Wilson Class: Definitions
The Wilson class consists of two discrete families (Racah and dual Hahn) and two continuous families (Wilson and continuous dual Hahn). …
Further Constraints for Racah Polynomials
§18.25(ii) Weights and Standardizations: Continuous Cases
§18.25(iii) Weights and Normalizations: Discrete Cases
12: 24.19 Methods of Computation
§24.19(i) Bernoulli and Euler Numbers and Polynomials
For algorithms for computing B n , E n , B n ( x ) , and E n ( x ) see Spanier and Oldham (1987, pp. 37, 41, 171, and 179–180).
§24.19(ii) Values of B n Modulo p
  • Buhler et al. (1992) uses the expansion

    24.19.3 t 2 cosh t 1 = 2 n = 0 ( 2 n 1 ) B 2 n t 2 n ( 2 n ) ! ,

    and computes inverses modulo p of the left-hand side. Multisectioning techniques are applied in implementations. See also Crandall (1996, pp. 116–120).

  • A method related to “Stickelberger codes” is applied in Buhler et al. (2001); in particular, it allows for an efficient search for the irregular pairs ( 2 n , p ) . Discrete Fourier transforms are used in the computations. See also Crandall (1996, pp. 120–124).

  • 13: 35.4 Partitions and Zonal Polynomials
    35.4.2 Z κ ( 𝐈 ) = | κ | !  2 2 | κ | [ m / 2 ] κ 1 j < l ( κ ) ( 2 k j 2 k l j + l ) j = 1 ( κ ) ( 2 k j + ( κ ) j ) !
    14: Bibliography K
  • T. Koornwinder, A. Kostenko, and G. Teschl (2018) Jacobi polynomials, Bernstein-type inequalities and dispersion estimates for the discrete Laguerre operator. Adv. Math. 333, pp. 796–821.
  • 15: Bibliography Y
  • H. A. Yamani and W. P. Reinhardt (1975) L -squared discretizations of the continuum: Radial kinetic energy and the Coulomb Hamiltonian. Phys. Rev. A 11 (4), pp. 1144–1156.
  • 16: Vadim B. Kuznetsov
    Kuznetsov published papers on special functions and orthogonal polynomials, the quantum scattering method, integrable discrete many-body systems, separation of variables, Bäcklund transformation techniques, and integrability in classical and quantum mechanics. …
    17: 18.12 Generating Functions
    18.12.2 𝐅 1 0 ( α + 1 ; ( x 1 ) z 2 ) 𝐅 1 0 ( β + 1 ; ( x + 1 ) z 2 ) = ( 1 2 ( 1 x ) z ) 1 2 α J α ( 2 ( 1 x ) z ) ( 1 2 ( 1 + x ) z ) 1 2 β I β ( 2 ( 1 + x ) z ) = n = 0 P n ( α , β ) ( x ) Γ ( n + α + 1 ) Γ ( n + β + 1 ) z n ,
    18: 18.30 Associated OP’s
    For other cases there may also be, in addition to a possible integral as in (18.30.10), a finite sum of discrete weights on the negative real x -axis each multiplied by the polynomial product evaluated at the corresponding values of x , as in (18.2.3). …
    19: 18.28 Askey–Wilson Class
    The Askey–Wilson polynomials form a system of OP’s { p n ( x ) } , n = 0 , 1 , 2 , , that are orthogonal with respect to a weight function on a bounded interval, possibly supplemented with discrete weights on a finite set. …
    20: 3.11 Approximation Techniques
    §3.11(ii) Chebyshev-Series Expansions
    Example. The Discrete Fourier Transform
    is called a discrete Fourier transform pair. … The direct computation of the discrete Fourier transform (3.11.38), that is, of … For splines based on Bernoulli and Euler polynomials, see §24.17(ii). …