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11: Bibliography
  • A. R. Ahmadi and S. E. Widnall (1985) Unsteady lifting-line theory as a singular-perturbation problem. J. Fluid Mech 153, pp. 59–81.
  • W. A. Al-Salam and L. Carlitz (1965) Some orthogonal q -polynomials. Math. Nachr. 30, pp. 47–61.
  • G. E. Andrews (2001) Bailey’s Transform, Lemma, Chains and Tree. In Special Functions 2000: Current Perspective and Future Directions (Tempe, AZ), J. Bustoz, M. E. H. Ismail, and S. K. Suslov (Eds.), NATO Sci. Ser. II Math. Phys. Chem., Vol. 30, pp. 1–22.
  • T. M. Apostol (1985b) Note on the trivial zeros of Dirichlet L -functions. Proc. Amer. Math. Soc. 94 (1), pp. 29–30.
  • V. I. Arnol’d (1975) Critical points of smooth functions, and their normal forms. Uspehi Mat. Nauk 30 (5(185)), pp. 3–65 (Russian).
  • 12: Bibliography T
  • J. D. Talman (1983) LSFBTR: A subroutine for calculating spherical Bessel transforms. Comput. Phys. Comm. 30 (1), pp. 93–99.
  • N. M. Temme (1979a) An algorithm with ALGOL 60 program for the computation of the zeros of ordinary Bessel functions and those of their derivatives. J. Comput. Phys. 32 (2), pp. 270–279.
  • N. M. Temme (1983) The numerical computation of the confluent hypergeometric function U ( a , b , z ) . Numer. Math. 41 (1), pp. 63–82.
  • H. Triebel (1965) Über die Lamésche Differentialgleichung. Math. Nachr. 30, pp. 137–154 (German).
  • 13: 29.21 Tables
  • Arscott and Khabaza (1962) tabulates the coefficients of the polynomials P in Table 29.12.1 (normalized so that the numerically largest coefficient is unity, i.e. monic polynomials), and the corresponding eigenvalues h for k 2 = 0.1 ( .1 ) 0.9 , n = 1 ( 1 ) 30 . Equations from §29.6 can be used to transform to the normalization adopted in this chapter. Precision is 6S.

  • 14: 31.18 Methods of Computation
    The computation of the accessory parameter for the Heun functions is carried out via the continued-fraction equations (31.4.2) and (31.11.13) in the same way as for the Mathieu, Lamé, and spheroidal wave functions in Chapters 2830.
    15: Peter A. Clarkson
     Kruskal), J. Math. Phys., 30 (1989) 2201–2213. …
    16: Hans Volkmer
    17: Bibliography F
  • B. R. Fabijonas, D. W. Lozier, and F. W. J. Olver (2004) Computation of complex Airy functions and their zeros using asymptotics and the differential equation. ACM Trans. Math. Software 30 (4), pp. 471–490.
  • B. R. Fabijonas (2004) Algorithm 838: Airy functions. ACM Trans. Math. Software 30 (4), pp. 491–501.
  • C. Ferreira, J. L. López, and E. Pérez Sinusía (2013a) The third Appell function for one large variable. J. Approx. Theory 165, pp. 60–69.
  • H. E. Fettis (1976) Complex roots of sin z = a z , cos z = a z , and cosh z = a z . Math. Comp. 30 (135), pp. 541–545.
  • A. S. Fokas and Y. C. Yortsos (1981) The transformation properties of the sixth Painlevé equation and one-parameter families of solutions. Lett. Nuovo Cimento (2) 30 (17), pp. 539–544.
  • 18: 24.1 Special Notation
    B 2 = 1 30 ,
    B 4 = 1 30 , .
    19: 24.20 Tables
    Wagstaff (1978) gives complete prime factorizations of N n and E n for n = 20 ( 2 ) 60 and n = 8 ( 2 ) 42 , respectively. In Wagstaff (2002) these results are extended to n = 60 ( 2 ) 152 and n = 40 ( 2 ) 88 , respectively, with further complete and partial factorizations listed up to n = 300 and n = 200 , respectively. …
    20: Bibliography S
  • F. W. Schäfke (1961a) Ein Verfahren zur Berechnung des charakteristischen Exponenten der Mathieuschen Differentialgleichung I. Numer. Math. 3 (1), pp. 30–38.
  • L. Schoenfeld (1976) Sharper bounds for the Chebyshev functions θ ( x ) and ψ ( x ) . II. Math. Comp. 30 (134), pp. 337–360.
  • L. J. Slater (1960) Confluent Hypergeometric Functions. Cambridge University Press, Cambridge-New York.
  • S. Yu. Slavyanov and N. A. Veshev (1997) Structure of avoided crossings for eigenvalues related to equations of Heun’s class. J. Phys. A 30 (2), pp. 673–687.
  • P. Spellucci and P. Pulay (1975) Effective calculation of the incomplete gamma function for parameter values α = ( 2 n + 1 ) / 2 , n = 0 , , 5 . Angew. Informatik 17, pp. 30–32.