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discrete q-Hermite I and II polynomials

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21: 18.2 General Orthogonal Polynomials
§18.2(ii) x -Difference Operators
§18.2(vi) Zeros
If d μ 𝐌 ( a , b ) then the interval [ b a , b + a ] is included in the support of d μ , and outside [ b a , b + a ] the measure d μ only has discrete mass points x k such that b ± a are the only possible limit points of the sequence { x k } , see Máté et al. (1991, Theorem 10). … The generating functions (18.12.13), (18.12.15), (18.23.3), (18.23.4), (18.23.5) and (18.23.7) for Laguerre, Hermite, Krawtchouk, Meixner, Charlier and Meixner–Pollaczek polynomials, respectively, can be written in the form (18.2.45). In fact, these are the only OP’s which are Sheffer polynomials (with Krawtchouk polynomials being only a finite system) …
22: Bibliography F
  • A. S. Fokas, B. Grammaticos, and A. Ramani (1993) From continuous to discrete Painlevé equations. J. Math. Anal. Appl. 180 (2), pp. 342–360.
  • 23: Bibliography N
  • G. Nemes (2013b) Error bounds and exponential improvement for Hermite’s asymptotic expansion for the gamma function. Appl. Anal. Discrete Math. 7 (1), pp. 161–179.
  • 24: 10.60 Sums
    10.60.3 e w w = 2 π n = 0 ( 2 n + 1 ) 𝗂 n ( 1 ) ( v ) 𝗄 n ( u ) P n ( cos α ) , | v e ± i α | < | u | .
    10.60.8 e z cos α = n = 0 ( 2 n + 1 ) 𝗂 n ( 1 ) ( z ) P n ( cos α ) ,
    10.60.9 e z cos α = n = 0 ( 1 ) n ( 2 n + 1 ) 𝗂 n ( 1 ) ( z ) P n ( cos α ) .
    25: 3.7 Ordinary Differential Equations
    §3.7(ii) Taylor-Series Method: Initial-Value Problems
    ( 𝐈 and 𝟎 being the identity and zero matrices of order 2 × 2 .) … 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 ) . … If q ( x ) is C on the closure of ( a , b ) , then the discretized form (3.7.13) of the differential equation can be used. This converts the problem into a tridiagonal matrix problem in which the elements of the matrix are polynomials in λ ; compare §3.2(vi). …
    26: Bibliography G
  • B. Gabutti and B. Minetti (1981) A new application of the discrete Laguerre polynomials in the numerical evaluation of the Hankel transform of a strongly decreasing even function. J. Comput. Phys. 42 (2), pp. 277–287.
  • 27: Bibliography S
  • A. Salem (2013) Some properties and expansions associated with the q -digamma function. Quaest. Math. 36 (1), pp. 67–77.
  • B. I. Schneider, X. Guan, and K. Bartschat (2016) Time propagation of partial differential equations using the short iterative Lanczos method and finite-element discrete variable representation. Adv. Quantum Chem. 72, pp. 95–127.
  • F. C. Smith (1939b) Relations among the fundamental solutions of the generalized hypergeometric equation when p = q + 1 . II. Logarithmic cases. Bull. Amer. Math. Soc. 45 (12), pp. 927–935.
  • W. F. Sun (1996) Uniform asymptotic expansions of Hermite polynomials. M. Phil. thesis, City University of Hong Kong.
  • G. Szegő (1975) Orthogonal Polynomials. 4th edition, Colloquium Publications, Vol. XXIII, American Mathematical Society, Providence, RI.
  • 28: 8.7 Series Expansions
    For the functions e n ( z ) , 𝗂 n ( 1 ) ( z ) , and L n ( α ) ( x ) see (8.4.11), §§10.47(ii), and 18.3, respectively. …
    29: Bibliography W
  • R. Wong and H. Y. Zhang (2009b) On the connection formulas of the third Painlevé transcendent. Discrete Contin. Dyn. Syst. 23 (1-2), pp. 541–560.
  • 30: 10.49 Explicit Formulas
    10.49.8 𝗂 n ( 1 ) ( z ) = 1 2 e z k = 0 n ( 1 ) k a k ( n + 1 2 ) z k + 1 + ( 1 ) n + 1 1 2 e z k = 0 n a k ( n + 1 2 ) z k + 1 .
    10.49.10 𝗂 n ( 2 ) ( z ) = 1 2 e z k = 0 n ( 1 ) k a k ( n + 1 2 ) z k + 1 + ( 1 ) n 1 2 e z k = 0 n a k ( n + 1 2 ) z k + 1 .