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31: 33.21 Asymptotic Approximations for Large | r |
§33.21 Asymptotic Approximations for Large | r |
§33.21(i) Limiting Forms
We indicate here how to obtain the limiting forms of f ( ϵ , ; r ) , h ( ϵ , ; r ) , s ( ϵ , ; r ) , and c ( ϵ , ; r ) as r ± , with ϵ and fixed, in the following cases: …
  • (c)

    When r ± with ϵ = 0 , combine (33.20.1), (33.20.2) with §§10.7(ii), 10.30(ii).

  • §33.21(ii) Asymptotic Expansions
    32: 2.1 Definitions and Elementary Properties
    Let 𝐗 be a point set with a limit point c . … If a s x s converges for all sufficiently large | x | , then it is automatically the asymptotic expansion of its sum as x in . If c is a finite limit point of 𝐗 , then … Similarly for finite limit point c in place of . … where c is a finite, or infinite, limit point of 𝐗 . …
    33: 2.4 Contour Integrals
    Except that λ is now permitted to be complex, with λ > 0 , we assume the same conditions on q ( t ) and also that the Laplace transform in (2.3.8) converges for all sufficiently large values of z . Then … For large t , the asymptotic expansion of q ( t ) may be obtained from (2.4.3) by Haar’s method. This depends on the availability of a comparison function F ( z ) for Q ( z ) that has an inverse transform …If this integral converges uniformly at each limit for all sufficiently large t , then by the Riemann–Lebesgue lemma (§1.8(i)) … in which z is a large real or complex parameter, p ( α , t ) and q ( α , t ) are analytic functions of t and continuous in t and a second parameter α . …
    34: 12.10 Uniform Asymptotic Expansions for Large Parameter
    §12.10 Uniform Asymptotic Expansions for Large Parameter
    §12.10(vi) Modifications of Expansions in Elementary Functions
    Modified Expansions
    35: 13.21 Uniform Asymptotic Approximations for Large κ
    §13.21 Uniform Asymptotic Approximations for Large κ
    §13.21(i) Large κ , Fixed μ
    §13.21(ii) Large κ , 0 μ ( 1 δ ) κ
    §13.21(iv) Large κ , Other Expansions
    36: 3.6 Linear Difference Equations
    Stability can be restored, however, by backward recursion, provided that c n 0 , n : starting from w N and w N + 1 , with N large, equation (3.6.3) is applied to generate in succession w N 1 , w N 2 , , w 0 . …
    37: 11.6 Asymptotic Expansions
    §11.6(i) Large | z | , Fixed ν
    §11.6(ii) Large | ν | , Fixed z
    §11.6(iii) Large | ν | , Fixed z / ν
    Here …These and higher coefficients c k ( λ ) can be computed via the representations in Nemes (2015b). …
    38: 1.17 Integral and Series Representations of the Dirac Delta
    More generally, assume ϕ ( x ) is piecewise continuous (§1.4(ii)) when x [ c , c ] for any finite positive real value of c , and for each a , e n ( x a ) 2 ϕ ( x ) d x converges absolutely for all sufficiently large values of n . …
    39: Bibliography K
  • K. W. J. Kadell (1994) A proof of the q -Macdonald-Morris conjecture for B C n . Mem. Amer. Math. Soc. 108 (516), pp. vi+80.
  • S. L. Kalla (1992) On the evaluation of the Gauss hypergeometric function. C. R. Acad. Bulgare Sci. 45 (6), pp. 35–36.
  • C. Kassel (1995) Quantum Groups. Graduate Texts in Mathematics, Vol. 155, Springer-Verlag, New York.
  • U. J. Knottnerus (1960) Approximation Formulae for Generalized Hypergeometric Functions for Large Values of the Parameters. J. B. Wolters, Groningen.
  • T. H. Koornwinder (1992) Askey-Wilson Polynomials for Root Systems of Type B C . In Hypergeometric Functions on Domains of Positivity, Jack Polynomials, and Applications (Tampa, FL, 1991), Contemp. Math., Vol. 138, pp. 189–204.
  • 40: 28.35 Tables
  • National Bureau of Standards (1967) includes the eigenvalues a n ( q ) , b n ( q ) for n = 0 ( 1 ) 3 with q = 0 ( .2 ) 20 ( .5 ) 37 ( 1 ) 100 , and n = 4 ( 1 ) 15 with q = 0 ( 2 ) 100 ; Fourier coefficients for ce n ( x , q ) and se n ( x , q ) for n = 0 ( 1 ) 15 , n = 1 ( 1 ) 15 , respectively, and various values of q in the interval [ 0 , 100 ] ; joining factors g e , n ( q ) , f e , n ( q ) for n = 0 ( 1 ) 15 with q = 0 ( .5  to  10 ) 100 (but in a different notation). Also, eigenvalues for large values of q . Precision is generally 8D.

  • Stratton et al. (1941) includes b n , b n , and the corresponding Fourier coefficients for Se n ( c , x ) and So n ( c , x ) for n = 0 or 1 ( 1 ) 4 , c = 0 ( .1 or .2 ) 4.5 . Precision is mostly 5S. Notation: c = 2 q , b n = a n + 2 q , b n = b n + 2 q , and for Se n ( c , x ) , So n ( c , x ) see §28.1.