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31: Bibliography O
  • A. B. Olde Daalhuis (2003a) Uniform asymptotic expansions for hypergeometric functions with large parameters. I. Analysis and Applications (Singapore) 1 (1), pp. 111–120.
  • A. B. Olde Daalhuis (2003b) Uniform asymptotic expansions for hypergeometric functions with large parameters. II. Analysis and Applications (Singapore) 1 (1), pp. 121–128.
  • A. B. Olde Daalhuis (2010) Uniform asymptotic expansions for hypergeometric functions with large parameters. III. Analysis and Applications (Singapore) 8 (2), pp. 199–210.
  • F. W. J. Olver (1951) A further method for the evaluation of zeros of Bessel functions and some new asymptotic expansions for zeros of functions of large order. Proc. Cambridge Philos. Soc. 47, pp. 699–712.
  • F. W. J. Olver (1975b) Legendre functions with both parameters large. Philos. Trans. Roy. Soc. London Ser. A 278, pp. 175–185.
  • 32: 12.2 Differential Equations
    12.2.1 d 2 w d z 2 + ( a z 2 + b z + c ) w = 0 ,
    Its importance is that when a is negative and | a | is large, U ( a , x ) and U ¯ ( a , x ) asymptotically have the same envelope (modulus) and are 1 2 π out of phase in the oscillatory interval 2 a < x < 2 a . …
    33: 18.2 General Orthogonal Polynomials
    Assume that the interval [ a , b ] is bounded. …
    The Nevai class 𝐌 ( a , b )
    For a large class of OP’s p n there exist pairs of differentiation formulas … For OP’s p n on [ a , b ] with weight function w ( x ) and orthogonality relation (18.2.5_5) assume that b < and w ( x ) is non-decreasing in the interval [ a , b ] . Then the functions w ( x ) p n ( x ) attain their maximum in [ a , b ] for x = b . …
    34: Bibliography S
  • J. B. Seaborn (1991) Hypergeometric Functions and Their Applications. Texts in Applied Mathematics, Vol. 8, Springer-Verlag, New York.
  • N. T. Shawagfeh (1992) The Laplace transforms of products of Airy functions. Dirāsāt Ser. B Pure Appl. Sci. 19 (2), pp. 7–11.
  • B. Simon (1982) Large orders and summability of eigenvalue perturbation theory: A mathematical overview. Int. J. Quantum Chem. 21, pp. 3–25.
  • B. Simon (2011) Szegő’s Theorem and Its Descendants. Spectral Theory for L 2 Perturbations of Orthogonal Polynomials. M. B. Porter Lectures, Princeton University Press, Princeton, NJ.
  • SLATEC (free Fortran library)
  • 35: Bibliography B
    Bibliography B
  • L. Baker (1992) C Mathematical Function Handbook. McGraw-Hill, Inc., New York.
  • C. M. Bender and T. T. Wu (1973) Anharmonic oscillator. II. A study of perturbation theory in large order. Phys. Rev. D 7, pp. 1620–1636.
  • L. C. Biedenharn, R. L. Gluckstern, M. H. Hull, and G. Breit (1955) Coulomb functions for large charges and small velocities. Phys. Rev. (2) 97 (2), pp. 542–554.
  • A. A. Bogush and V. S. Otchik (1997) Problem of two Coulomb centres at large intercentre separation: Asymptotic expansions from analytical solutions of the Heun equation. J. Phys. A 30 (2), pp. 559–571.
  • 36: 2.5 Mellin Transform Methods
    with a < c < b . … where a < c < b . … where J ν denotes the Bessel function (§10.2(ii)), and x is a large positive parameter. … From (2.5.12) and (2.5.13), it is seen that a s = b s = 0 when s is even. … for z < b . …
    37: 3.8 Nonlinear Equations
    for all n sufficiently large, where A and p are independent of n , then the sequence is said to have convergence of the p th order. …
  • (b)

    f ( x 0 ) f ′′ ( x 0 ) < 0 , f ( x ) , f ′′ ( x ) do not change sign in the interval ( x 0 , x 1 ) , and ξ [ x 0 , x 1 ] (monotonic convergence after the first iteration).

  • If f ( a ) f ( b ) < 0 with a < b , then the interval [ a , b ] contains one or more zeros of f . …All zeros of f in the original interval [ a , b ] can be computed to any predetermined accuracy. …
    38: 33.9 Expansions in Series of Bessel Functions
    33.9.3 F ( η , ρ ) = C ( η ) ( 2 + 1 ) ! ( 2 η ) 2 + 1 ρ k = 2 + 1 b k t k / 2 I k ( 2 t ) , η > 0 ,
    33.9.4 F ( η , ρ ) = C ( η ) ( 2 + 1 ) ! ( 2 | η | ) 2 + 1 ρ k = 2 + 1 b k t k / 2 J k ( 2 t ) , η < 0 .
    Here b 2 = b 2 + 2 = 0 , b 2 + 1 = 1 , and
    33.9.5 4 η 2 ( k 2 ) b k + 1 + k b k 1 + b k 2 = 0 , k = 2 + 2 , 2 + 3 , .
    33.9.7 λ ( η ) k = 2 + 1 ( 1 ) k ( k 1 ) ! b k .
    39: 36.12 Uniform Approximation of Integrals
    where k is a large real parameter and 𝐲 = { y 1 , y 2 , } is a set of additional (nonasymptotic) parameters. …
    40: Ronald F. Boisvert
    Ronald F. Boisvert (b. …