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31: 10.75 Tables
  • Olver (1962) provides tables for the uniform asymptotic expansions given in §10.20(i), including ζ and ( 4 ζ / ( 1 x 2 ) ) 1 4 as functions of x ( = z ) and the coefficients A k ( ζ ) , B k ( ζ ) , C k ( ζ ) , D k ( ζ ) as functions of ζ . These enable J ν ( ν x ) , Y ν ( ν x ) , J ν ( ν x ) , Y ν ( ν x ) to be computed to 10S when ν 15 , except in the neighborhoods of zeros.

  • Olver (1962) provides tables for the uniform asymptotic expansions given in §10.41(ii), including η and the coefficients U k ( p ) , V k ( p ) as functions of p = ( 1 + x 2 ) 1 2 . These enable I ν ( ν x ) , K ν ( ν x ) , I ν ( ν x ) , K ν ( ν x ) to be computed to 10S when ν 16 .

  • 32: 23.22 Methods of Computation
    §23.22 Methods of Computation
    The functions ζ ( z ) and σ ( z ) are computed in a similar manner: the former by replacing u and z in (23.6.13) by z and π z / ( 2 ω 1 ) , respectively, and also referring to (23.6.8); the latter by applying (23.6.9). …
    §23.22(ii) Lattice Calculations
    Suppose that the invariants g 2 = c , g 3 = d , are given, for example in the differential equation (23.3.10) or via coefficients of an elliptic curve (§23.20(ii)). …
    33: Bibliography J
  • L. Jacobsen, W. B. Jones, and H. Waadeland (1986) Further results on the computation of incomplete gamma functions. In Analytic Theory of Continued Fractions, II (Pitlochry/Aviemore, 1985), W. J. Thron (Ed.), Lecture Notes in Math. 1199, pp. 67–89.
  • M. Jimbo and T. Miwa (1981) Monodromy preserving deformation of linear ordinary differential equations with rational coefficients. II. Phys. D 2 (3), pp. 407–448.
  • F. Johansson (2012) Efficient implementation of the Hardy-Ramanujan-Rademacher formula. LMS J. Comput. Math. 15, pp. 341–359.
  • D. S. Jones (2006) Parabolic cylinder functions of large order. J. Comput. Appl. Math. 190 (1-2), pp. 453–469.
  • W. B. Jones and W. J. Thron (1985) On the computation of incomplete gamma functions in the complex domain. J. Comput. Appl. Math. 12/13, pp. 401–417.
  • 34: 30.18 Software
    A more complete list of available software for computing these functions is found in the Software Index. …
  • SWF7: Coefficients β p in (30.9.1).

  • SWF8: Coefficients c p in (30.9.4).

  • SWF9: Coefficients p in (30.3.8).

  • 35: Bibliography W
  • E. L. Wachspress (2000) Evaluating elliptic functions and their inverses. Comput. Math. Appl. 39 (3-4), pp. 131–136.
  • E. J. Weniger (1996) Computation of the Whittaker function of the second kind by summing its divergent asymptotic series with the help of nonlinear sequence transformations. Computers in Physics 10 (5), pp. 496–503.
  • J. Wimp (1984) Computation with Recurrence Relations. Pitman, Boston, MA.
  • M. E. Wojcicki (1961) Algorithm 44: Bessel functions computed recursively. Comm. ACM 4 (4), pp. 177–178.
  • G. Wolf (2008) On the asymptotic behavior of the Fourier coefficients of Mathieu functions. J. Res. Nat. Inst. Standards Tech. 113 (1), pp. 11–15.
  • 36: 10.21 Zeros
    For the first zeros rounded numerical values of the coefficients are given by … For numerical coefficients for m = 2 , 3 , 4 , 5 see Olver (1951, Tables 3–6). … The latter reference includes numerical tables of the first few coefficients in the uniform asymptotic expansions. … Higher coefficients in the asymptotic expansions in this subsection can be obtained by expressing the cross-products in terms of the modulus and phase functions (§10.18), and then reverting the asymptotic expansion for the difference of the phase functions. … For properties, computation, and generalizations see Kapitsa (1951b), Kerimov (1999, 2008), and Gupta and Muldoon (2000). …
    37: 3.5 Quadrature
    which depends on function values computed previously. … can be computed by Filon’s rule. …
    Example
    38: 29.7 Asymptotic Expansions
    29.7.1 a ν m ( k 2 ) p κ τ 0 τ 1 κ 1 τ 2 κ 2 ,
    29.7.3 τ 0 = 1 2 3 ( 1 + k 2 ) ( 1 + p 2 ) ,
    29.7.4 τ 1 = p 2 6 ( ( 1 + k 2 ) 2 ( p 2 + 3 ) 4 k 2 ( p 2 + 5 ) ) .
    29.7.6 τ 2 = 1 2 10 ( 1 + k 2 ) ( 1 k 2 ) 2 ( 5 p 4 + 34 p 2 + 9 ) ,
    Formulas for additional terms can be computed with the author’s Maple program LA5; see §29.22. …
    39: 3.8 Nonlinear Equations
    §3.8 Nonlinear Equations
    All zeros of f in the original interval [ a , b ] can be computed to any predetermined accuracy. …
    §3.8(iv) Zeros of Polynomials
    However, when the coefficients are all real, complex arithmetic can be avoided by the following iterative process. … For further information on the computation of zeros of polynomials see McNamee (2007). …
    40: 26.6 Other Lattice Path Numbers
    26.6.1 D ( m , n ) = k = 0 n ( n k ) ( m + n k n ) = k = 0 n 2 k ( m k ) ( n k ) .
    26.6.2 M ( n ) = k = 0 n ( 1 ) k n + 2 k ( n k ) ( 2 n + 2 2 k n + 1 k ) .
    26.6.3 N ( n , k ) = 1 n ( n k ) ( n k 1 ) .
    26.6.13 M ( n ) = k = 0 n ( 1 ) k ( n k ) C ( n + 1 k ) ,
    26.6.14 C ( n ) = k = 0 2 n ( 1 ) k ( 2 n k ) M ( 2 n k ) .