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11: 30.9 Asymptotic Approximations and Expansions
§30.9(i) Prolate Spheroidal Wave Functions
For uniform asymptotic expansions in terms of Airy or Bessel functions for real values of the parameters, complex values of the variable, and with explicit error bounds see Dunster (1986). …
§30.9(ii) Oblate Spheroidal Wave Functions
§30.9(iii) Other Approximations and Expansions
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). …
12: 2.11 Remainder Terms; Stokes Phenomenon
If we permit the use of nonelementary functions as approximants, then even more powerful re-expansions become available. … These answers are linked to the terms involving the complementary error function in the more powerful expansions typified by the combination of (2.11.10) and (2.11.15). … The first of these two references also provides an introduction to the powerful Borel transform theory. … The following example, based on Weniger (1996), illustrates their power. … For example, using double precision d 20 is found to agree with (2.11.31) to 13D. …
13: Bibliography K
  • P. L. Kapitsa (1951b) The computation of the sums of negative even powers of roots of Bessel functions. Doklady Akad. Nauk SSSR (N.S.) 77, pp. 561–564.
  • R. B. Kearfott, M. Dawande, K. Du, and C. Hu (1994) Algorithm 737: INTLIB: A portable Fortran 77 interval standard-function library. ACM Trans. Math. Software 20 (4), pp. 447–459.
  • M. K. Kerimov (1980) Methods of computing the Riemann zeta-function and some generalizations of it. USSR Comput. Math. and Math. Phys. 20 (6), pp. 212–230.
  • A. V. Kitaev and A. H. Vartanian (2004) Connection formulae for asymptotics of solutions of the degenerate third Painlevé equation. I. Inverse Problems 20 (4), pp. 1165–1206.
  • T. H. Koornwinder (2009) The Askey scheme as a four-manifold with corners. Ramanujan J. 20 (3), pp. 409–439.
  • 14: 18.40 Methods of Computation
    Given the power moments, μ n = a b x n d μ ( x ) , n = 0 , 1 , 2 , , can these be used to find a unique μ ( x ) , a non-decreasing, real, function of x , in the case that the moment problem is determined? Should a unique solution not exist the moment problem is then indeterminant. … Results of low ( 2 to 3 decimal digits) precision for w ( x ) are easily obtained for N 10 to 20 . … H ( x ) being the Heaviside step-function, see (1.16.13). … The example chosen is inversion from the α n , β n for the weight function for the repulsive Coulomb–Pollaczek, RCP, polynomials of (18.39.50). … Further, exponential convergence in N , via the Derivative Rule, rather than the power-law convergence of the histogram methods, is found for the inversion of Gegenbauer, Attractive, as well as Repulsive, Coulomb–Pollaczek, and Hermite weights and zeros to approximate w ( x ) for these OP systems on x [ 1 , 1 ] and ( , ) respectively, Reinhardt (2018), and Reinhardt (2021b), Reinhardt (2021a). …