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as eigenfunctions of a q-difference operator

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11: 28.12 Definitions and Basic Properties
As a function of ν with fixed q ( 0 ), λ ν ( q ) is discontinuous at ν = ± 1 , ± 2 , . …
§28.12(ii) Eigenfunctions me ν ( z , q )
Two eigenfunctions correspond to each eigenvalue a = λ ν ( q ) . …The other eigenfunction is me ν ( z , q ) , a Floquet solution with respect to ν with a = λ ν ( q ) . If q is a normal value of the corresponding equation (28.2.16), then these functions are uniquely determined as analytic functions of z and q by the normalization …
12: Bibliography K
  • T. H. Koornwinder (2006) Lowering and Raising Operators for Some Special Orthogonal Polynomials. In Jack, Hall-Littlewood and Macdonald Polynomials, Contemp. Math., Vol. 417, pp. 227–238.
  • T. H. Koornwinder (2015) Fractional integral and generalized Stieltjes transforms for hypergeometric functions as transmutation operators. SIGMA Symmetry Integrability Geom. Methods Appl. 11, pp. Paper 074, 22.
  • 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.
  • C. Kormanyos (2011) Algorithm 910: a portable C++ multiple-precision system for special-function calculations. ACM Trans. Math. Software 37 (4), pp. Art. 45, 27.
  • K. H. Kwon, L. L. Littlejohn, and G. J. Yoon (2006) Construction of differential operators having Bochner-Krall orthogonal polynomials as eigenfunctions. J. Math. Anal. Appl. 324 (1), pp. 285–303.
  • 13: 29.3 Definitions and Basic Properties
    They are denoted by a ν 2 m ( k 2 ) , a ν 2 m + 1 ( k 2 ) , b ν 2 m + 1 ( k 2 ) , b ν 2 m + 2 ( k 2 ) , where m = 0 , 1 , 2 , ; see Table 29.3.1. … If ν is a nonnegative integer, then … If ν is a nonnegative integer and 2 p > ν , then (29.3.10) has only the solutions (29.3.9) with 2 m > ν . … The eigenfunctions corresponding to the eigenvalues of §29.3(i) are denoted by 𝐸𝑐 ν 2 m ( z , k 2 ) , 𝐸𝑐 ν 2 m + 1 ( z , k 2 ) , 𝐸𝑠 ν 2 m + 1 ( z , k 2 ) , 𝐸𝑠 ν 2 m + 2 ( z , k 2 ) . …
    14: 3.7 Ordinary Differential Equations
    where 𝐀 ( τ , z ) is the matrix … Let ( a , b ) be a finite or infinite interval and q ( x ) be a real-valued continuous (or piecewise continuous) function on the closure of ( a , b ) . The Sturm–Liouville eigenvalue problem is the construction of a nontrivial solution of the system …The values λ k are the eigenvalues and the corresponding solutions w k of the differential equation are the eigenfunctions. The eigenvalues λ k are simple, that is, there is only one corresponding eigenfunction (apart from a normalization factor), and when ordered increasingly the eigenvalues satisfy …
    15: 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. … y ) such that P n ( z ) = p n ( 1 2 ( z + z 1 ) ) in the Askey–Wilson case, and P n ( y ) = p n ( q y + c q y + 1 ) in the q -Racah case, and both are eigenfunctions of a second order q -difference operator similar to (18.27.1). … where the operator L is defined by … In Tsujimoto et al. (2012) an extension of the Bannai–Ito polynomials occurs as eigenfunctions of a Dunkl type operator. …
    16: DLMF Project News
    error generating summary
    17: 30.9 Asymptotic Approximations and Expansions
    For the eigenfunctions see Meixner and Schäfke (1954, §3.251) and Müller (1963). … For the eigenfunctions see Meixner and Schäfke (1954, §3.252) and Müller (1962). … The asymptotic behavior of λ n m ( γ 2 ) and a n , k m ( γ 2 ) as n in descending powers of 2 n + 1 is derived in Meixner (1944). …
    18: Bibliography J
  • L. Jager (1998) Fonctions de Mathieu et fonctions propres de l’oscillateur relativiste. Ann. Fac. Sci. Toulouse Math. (6) 7 (3), pp. 465–495 (French).
  • A. J. Jerri (1982) A note on sampling expansion for a transform with parabolic cylinder kernel. Inform. Sci. 26 (2), pp. 155–158.
  • J. H. Johnson and J. M. Blair (1973) REMES2 — a Fortran program to calculate rational minimax approximations to a given function. Technical Report Technical Report AECL-4210, Atomic Energy of Canada Limited. Chalk River Nuclear Laboratories, Chalk River, Ontario.
  • D. S. Jones (1997) Introduction to Asymptotics: A Treatment Using Nonstandard Analysis. World Scientific Publishing Co. Inc., River Edge, NJ.
  • B. R. Judd (1998) Operator Techniques in Atomic Spectroscopy. Princeton University Press, Princeton, NJ.
  • 19: Bibliography V
  • Van Buren (website) Mathieu and Spheroidal Wave Functions: Fortran Programs for their Accurate Calculation
  • N. Ja. Vilenkin and A. U. Klimyk (1991) Representation of Lie Groups and Special Functions. Volume 1: Simplest Lie Groups, Special Functions and Integral Transforms. Mathematics and its Applications (Soviet Series), Vol. 72, Kluwer Academic Publishers Group, Dordrecht.
  • N. Ja. Vilenkin and A. U. Klimyk (1992) Representation of Lie Groups and Special Functions. Volume 3: Classical and Quantum Groups and Special Functions. Mathematics and its Applications (Soviet Series), Vol. 75, Kluwer Academic Publishers Group, Dordrecht.
  • N. Ja. Vilenkin and A. U. Klimyk (1993) Representation of Lie Groups and Special Functions. Volume 2: Class I Representations, Special Functions, and Integral Transforms. Mathematics and its Applications (Soviet Series), Vol. 74, Kluwer Academic Publishers Group, Dordrecht.
  • H. Volkmer (2004a) Error estimates for Rayleigh-Ritz approximations of eigenvalues and eigenfunctions of the Mathieu and spheroidal wave equation. Constr. Approx. 20 (1), pp. 39–54.
  • 20: 1.17 Integral and Series Representations of the Dirac Delta
    This is a symbolic function with the properties: …Such a sequence is called a delta sequence and we write, symbolically, … An example of a delta sequence is provided by … For a generalization of (1.17.14) see Maximon (1991). … In the language of physics and applied mathematics, these equations indicate the normalizations chosen for these non- L 2 improper eigenfunctions of the differential operators (with derivatives respect to spatial co-ordinates) which generate them; the normalizations (1.17.12_1) and (1.17.12_2) are explicitly derived in Friedman (1990, Ch. 4), the others follow similarly. …