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11: 2.11 Remainder Terms; Stokes Phenomenon
with … … However, to enjoy the resurgence property (§2.7(ii)) we often seek instead expansions in terms of the F -functions introduced in §2.11(iii), leaving the connection of the error-function type behavior as an implicit consequence of this property of the F -functions. … in which …
12: 2.7 Differential Equations
is one at which the coefficients f ( z ) and g ( z ) are analytic. … Formal solutions are … Note that the coefficients in the expansions (2.7.12), (2.7.13) for the “late” coefficients, that is, a s , 1 , a s , 2 with s large, are the “early” coefficients a j , 2 , a j , 1 with j small. …See §2.11(v) for other examples. … For irregular singularities of nonclassifiable rank, a powerful tool for finding the asymptotic behavior of solutions, complete with error bounds, is as follows: …
13: 2.3 Integrals of a Real Variable
For the Fourier integral … Other types of singular behavior in the integrand can be treated in an analogous manner. …
  • (b)

    As t a +

    2.3.14
    p ( t ) p ( a ) + s = 0 p s ( t a ) s + μ ,
    q ( t ) s = 0 q s ( t a ) s + λ 1 ,

    and the expansion for p ( t ) is differentiable. Again λ and μ are positive constants. Also p 0 > 0 (consistent with (a)).

  • Then …
    §2.3(vi) Asymptotics of Mellin Transforms
    14: Bibliography K
  • T. A. Kaeding (1995) Pascal program for generating tables of SU ( 3 ) Clebsch-Gordan coefficients. Comput. Phys. Comm. 85 (1), pp. 82–88.
  • A. A. Kapaev (1988) Asymptotic behavior of the solutions of the Painlevé equation of the first kind. Differ. Uravn. 24 (10), pp. 1684–1695 (Russian).
  • D. Karp and S. M. Sitnik (2007) Asymptotic approximations for the first incomplete elliptic integral near logarithmic singularity. J. Comput. Appl. Math. 205 (1), pp. 186–206.
  • T. H. Koornwinder (1981) Clebsch-Gordan coefficients for SU ( 2 ) and Hahn polynomials. Nieuw Arch. Wisk. (3) 29 (2), pp. 140–155.
  • Y. A. Kravtsov (1964) Asymptotic solution of Maxwell’s equations near caustics. Izv. Vuz. Radiofiz. 7, pp. 1049–1056.
  • 15: 3.5 Quadrature
    The w k are also known as Christoffel coefficients or Christoffel numbers and they are all positive. The remainder is given by … In practical applications the weight function w ( x ) is chosen to simulate the asymptotic behavior of the integrand as the endpoints are approached. … Below we give for the classical orthogonal polynomials the recurrence coefficients α n and β n in (3.5.30). These also immediately yield the recurrence coefficients in (3.5.30_5). …
    16: 18.2 General Orthogonal Polynomials
    Then, with the coefficients (18.2.11_4) associated with the monic OP’s p n , the orthonormal recurrence relation for q n takes the form … The monic and orthonormal OP’s, and their determination via recursion, are more fully discussed in §§3.5(v) and 3.5(vi), where modified recursion coefficients are listed for the classical OP’s in their monic and orthonormal forms. … Alternatives for numerical calculation of the recursion coefficients in terms of the moments are discussed in these references, and in §18.40(ii). … This says roughly that the series (18.2.25) has the same pointwise convergence behavior as the same series with p n ( x ) = T n ( x ) , a Chebyshev polynomial of the first kind, see Table 18.3.1. … for certain coefficients a n , j with s , t independent of n . …
    17: 30.11 Radial Spheroidal Wave Functions
    §30.11(iii) Asymptotic Behavior
    For asymptotic expansions in negative powers of z see Meixner and Schäfke (1954, p. 293). … where
    30.11.10 K n m ( γ ) = π 2 ( γ 2 ) m ( 1 ) m a n , 1 2 ( m n ) m ( γ 2 ) Γ ( 3 2 + m ) A n m ( γ 2 ) 𝖯𝗌 n m ( 0 , γ 2 ) , n m even,
    30.11.11 K n m ( γ ) = π 2 ( γ 2 ) m + 1 ( 1 ) m a n , 1 2 ( m n + 1 ) m ( γ 2 ) Γ ( 5 2 + m ) A n m ( γ 2 ) ( d 𝖯𝗌 n m ( z , γ 2 ) / d z | z = 0 ) , n m odd.
    18: 18.15 Asymptotic Approximations
    §18.15 Asymptotic Approximations
    §18.15(i) Jacobi
    §18.15(ii) Ultraspherical
    The leading coefficients are given by … The asymptotic behavior of the classical OP’s as x ± with the degree and parameters fixed is evident from their explicit polynomial forms; see, for example, (18.2.7) and the last two columns of Table 18.3.1. …
    19: 25.11 Hurwitz Zeta Function
    §25.11(xii) a -Asymptotic Behavior
    As a in the sector | ph a | π δ ( < π ) , with s ( 1 ) and δ fixed, we have the asymptotic expansion … Similarly, as a in the sector | ph a | 1 2 π δ ( < 1 2 π ) ,
    25.11.44 ζ ( 1 , a ) 1 12 + 1 4 a 2 ( 1 12 1 2 a + 1 2 a 2 ) ln a k = 1 B 2 k + 2 ( 2 k + 2 ) ( 2 k + 1 ) 2 k a 2 k ,
    25.11.45 ζ ( 2 , a ) 1 12 a + 1 9 a 3 ( 1 6 a 1 2 a 2 + 1 3 a 3 ) ln a k = 1 2 B 2 k + 2 ( 2 k + 2 ) ( 2 k + 1 ) 2 k ( 2 k 1 ) a ( 2 k 1 ) .
    20: 15.12 Asymptotic Approximations
    §15.12 Asymptotic Approximations
    §15.12(i) Large Variable
    For the asymptotic behavior of 𝐅 ( a , b ; c ; z ) as z with a , b , c fixed, combine (15.2.2) with (15.8.2) or (15.8.8).
    §15.12(ii) Large c
    For other extensions, see Wagner (1986), Temme (2003) and Temme (2015, Chapters 12 and 28).