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11: Bibliography
  • M. Abramowitz (1949) Asymptotic expansions of spheroidal wave functions. J. Math. Phys. Mass. Inst. Tech. 28, pp. 195–199.
  • S. Ahmed and M. E. Muldoon (1980) On the zeros of confluent hypergeometric functions. III. Characterization by means of nonlinear equations. Lett. Nuovo Cimento (2) 29 (11), pp. 353–358.
  • D. E. Amos (1983a) Algorithm 609. A portable FORTRAN subroutine for the Bickley functions Ki n ( x ) . ACM Trans. Math. Software 9 (4), pp. 480–493.
  • D. E. Amos (1983c) Uniform asymptotic expansions for exponential integrals E n ( x ) and Bickley functions Ki n ( x ) . ACM Trans. Math. Software 9 (4), pp. 467–479.
  • V. I. Arnol’d (1974) Normal forms of functions in the neighborhood of degenerate critical points. Uspehi Mat. Nauk 29 (2(176)), pp. 11–49 (Russian).
  • 12: 18.8 Differential Equations
    Table 18.8.1: Classical OP’s: differential equations A ( x ) f ′′ ( x ) + B ( x ) f ( x ) + C ( x ) f ( x ) + λ n f ( x ) = 0 .
    # f ( x ) A ( x ) B ( x ) C ( x ) λ n
    9 e 1 2 x 2 x α + 1 2 L n ( α ) ( x 2 ) 1 0 x 2 + ( 1 4 α 2 ) x 2 4 n + 2 α + 2
    11 e n 1 x x + 1 L n 1 ( 2 + 1 ) ( 2 n 1 x ) 1 0 2 x ( + 1 ) x 2 1 n 2
    12 H n ( x ) 1 2 x 0 2 n
    Item 11 of Table 18.8.1 yields (18.39.36) for Z = 1 .
    13: 24.2 Definitions and Generating Functions
    B 2 n + 1 = 0 ,
    24.2.4 B n = B n ( 0 ) ,
    Table 24.2.4: Euler numbers E n .
    n E n
    Table 24.2.5: Coefficients b n , k of the Bernoulli polynomials B n ( x ) = k = 0 n b n , k x k .
    k
    Table 24.2.6: Coefficients e n , k of the Euler polynomials E n ( x ) = k = 0 n e n , k x k .
    k
    14: 26.12 Plane Partitions
    26.12.9 ( h = 1 r j = 1 s h + j + t 1 h + j 1 ) 2 ;
    26.12.10 ( h = 1 r j = 1 s h + j + t 1 h + j 1 ) ( h = 1 r + 1 j = 1 s h + j + t 1 h + j 1 ) ;
    26.12.11 ( h = 1 r + 1 j = 1 s h + j + t 1 h + j 1 ) ( h = 1 r j = 1 s + 1 h + j + t 1 h + j 1 ) .
    The notation π B ( r , s , t ) denotes the sum over all plane partitions contained in B ( r , s , t ) , and | π | denotes the number of elements in π . … where σ 2 ( j ) is the sum of the squares of the divisors of j . …
    15: Bibliography E
  • C. Eckart (1930) The penetration of a potential barrier by electrons. Phys. Rev. 35 (11), pp. 1303–1309.
  • F. H. L. Essler, H. Frahm, A. R. Its, and V. E. Korepin (1996) Painlevé transcendent describes quantum correlation function of the X X Z antiferromagnet away from the free-fermion point. J. Phys. A 29 (17), pp. 5619–5626.
  • L. Euler (1768) Institutiones Calculi Integralis. Opera Omnia (1), Vol. 11, pp. 110–113.
  • W. N. Everitt, L. L. Littlejohn, and R. Wellman (2004) The Sobolev orthogonality and spectral analysis of the Laguerre polynomials { L n k } for positive integers k . J. Comput. Appl. Math. 171 (1-2), pp. 199–234.
  • W. N. Everitt (2008) Note on the X 1 -Laguerre orthogonal polynomials.
  • 16: 4.17 Special Values and Limits
    Table 4.17.1: Trigonometric functions: values at multiples of 1 12 π .
    θ sin θ cos θ tan θ csc θ sec θ cot θ
    11 π / 12 1 4 2 ( 3 1 ) 1 4 2 ( 3 + 1 ) ( 2 3 ) 2 ( 3 + 1 ) 2 ( 3 1 ) ( 2 + 3 )
    4.17.1 lim z 0 sin z z = 1 ,
    4.17.2 lim z 0 tan z z = 1 .
    4.17.3 lim z 0 1 cos z z 2 = 1 2 .
    17: Bibliography K
  • G. A. Kalugin, D. J. Jeffrey, and R. M. Corless (2012) Bernstein, Pick, Poisson and related integral expressions for Lambert W . Integral Transforms Spec. Funct. 23 (11), pp. 817–829.
  • E. L. Kaplan (1948) Auxiliary table for the incomplete elliptic integrals. J. Math. Physics 27, pp. 11–36.
  • S. K. Kim (1972) The asymptotic expansion of a hypergeometric function F 2 2 ( 1 , α ; ρ 1 , ρ 2 ; z ) . Math. Comp. 26 (120), pp. 963.
  • Y. S. Kim, A. K. Rathie, and R. B. Paris (2013) An extension of Saalschütz’s summation theorem for the series F r + 2 r + 3 . Integral Transforms Spec. Funct. 24 (11), pp. 916–921.
  • K. S. Kölbig (1968) Algorithm 327: Dilogarithm [S22]. Comm. ACM 11 (4), pp. 270–271.
  • 18: Bibliography L
  • A. Leitner and J. Meixner (1960) Eine Verallgemeinerung der Sphäroidfunktionen. Arch. Math. 11, pp. 29–39.
  • M. Lerch (1887) Note sur la fonction 𝔎 ( w , x , s ) = k = 0 e 2 k π i x ( w + k ) s . Acta Math. 11 (1-4), pp. 19–24 (French).
  • J. L. López, P. Pagola, and E. Pérez Sinusía (2013b) Asymptotics of the first Appell function F 1 with large parameters. Integral Transforms Spec. Funct. 24 (9), pp. 715–733.
  • H. Lotsch and M. Gray (1964) Algorithm 244: Fresnel integrals. Comm. ACM 7 (11), pp. 660–661.
  • N. A. Lukaševič (1967b) On the theory of Painlevé’s third equation. Differ. Uravn. 3 (11), pp. 1913–1923 (Russian).
  • 19: Bibliography O
  • K. Okamoto (1986) Studies on the Painlevé equations. III. Second and fourth Painlevé equations, P II and P IV . Math. Ann. 275 (2), pp. 221–255.
  • A. B. Olde Daalhuis (1998a) Hyperasymptotic solutions of higher order linear differential equations with a singularity of rank one. Proc. Roy. Soc. London Ser. A 454, pp. 1–29.
  • F. W. J. Olver (1974) Error bounds for stationary phase approximations. SIAM J. Math. Anal. 5 (1), pp. 19–29.
  • S. Olver (2011) Numerical solution of Riemann-Hilbert problems: Painlevé II. Found. Comput. Math. 11 (2), pp. 153–179.
  • H. Oser (1960) Algorithm 22: Riccati-Bessel functions of first and second kind. Comm. ACM 3 (11), pp. 600–601.
  • 20: Staff
  • Frank W. J. Olver, University of Maryland and NIST, Chaps. 1, 2, 4, 9, 10

  • Richard B. Paris, University of Abertay, Chaps. 8, 11

  • Hans Volkmer, University of Wisconsin, Milwaukee, Chaps. 29, 30

  • Richard B. Paris, University of Abertay Dundee, for Chaps. 8, 11 (deceased)

  • Hans Volkmer, University of Wisconsin–Milwaukee, for Chaps. 29, 30