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41: Bibliography B
  • M. V. Berry and C. J. Howls (1993) Unfolding the high orders of asymptotic expansions with coalescing saddles: Singularity theory, crossover and duality. Proc. Roy. Soc. London Ser. A 443, pp. 107–126.
  • M. V. Berry (1981) Singularities in Waves and Rays. In Les Houches Lecture Series Session XXXV, R. Balian, M. Kléman, and J.-P. Poirier (Eds.), Vol. 35, pp. 453–543.
  • N. Bleistein (1966) Uniform asymptotic expansions of integrals with stationary point near algebraic singularity. Comm. Pure Appl. Math. 19, pp. 353–370.
  • N. Bleistein (1967) Uniform asymptotic expansions of integrals with many nearby stationary points and algebraic singularities. J. Math. Mech. 17, pp. 533–559.
  • W. G. C. Boyd and T. M. Dunster (1986) Uniform asymptotic solutions of a class of second-order linear differential equations having a turning point and a regular singularity, with an application to Legendre functions. SIAM J. Math. Anal. 17 (2), pp. 422–450.
  • 42: 1.13 Differential Equations
    §1.13(vi) Singularities
    For classification of singularities of (1.13.1) and expansions of solutions in the neighborhoods of singularities, see §2.7. …
    43: 2.4 Contour Integrals
    The problems sketched in §§2.3(v) and 2.4(v) involve only two of many possibilities for the coalescence of endpoints, saddle points, and singularities in integrals associated with the special functions. …For a coalescing saddle point and endpoint see Olver (1997b, Chapter 9) and Wong (1989, Chapter 7); if the endpoint is an algebraic singularity then the uniform approximants are parabolic cylinder functions with fixed parameter, and if the endpoint is not a singularity then the uniform approximants are complementary error functions. … For two coalescing saddle points and an algebraic singularity see Temme (1986), Jin and Wong (1998). …
    44: 10.47 Definitions and Basic Properties
    Equations (10.47.1) and (10.47.2) each have a regular singularity at z = 0 with indices n , n 1 , and an irregular singularity at z = of rank 1 ; compare §§2.7(i)2.7(ii). …
    45: 20.13 Physical Applications
    In the singular limit τ 0 + , the functions θ j ( z | τ ) , j = 1 , 2 , 3 , 4 , become integral kernels of Feynman path integrals (distribution-valued Green’s functions); see Schulman (1981, pp. 194–195). …
    46: 28.7 Analytic Continuation of Eigenvalues
    The only singularities are algebraic branch points, with a n ( q ) and b n ( q ) finite at these points. …
    47: Bibliography F
  • F. Feuillebois (1991) Numerical calculation of singular integrals related to Hankel transform. Comput. Math. Appl. 21 (2-3), pp. 87–94.
  • P. Flajolet and A. Odlyzko (1990) Singularity analysis of generating functions. SIAM J. Discrete Math. 3 (2), pp. 216–240.
  • 48: Bibliography W
  • R. Wong and J. F. Lin (1978) Asymptotic expansions of Fourier transforms of functions with logarithmic singularities. J. Math. Anal. Appl. 64 (1), pp. 173–180.
  • R. Wong (1977) Asymptotic expansions of Hankel transforms of functions with logarithmic singularities. Comput. Math. Appl. 3 (4), pp. 271–286.
  • 49: 15.2 Definitions and Analytical Properties
    §15.2(ii) Analytic Properties
    50: Bibliography E
  • A. Erdélyi (1942b) The Fuchsian equation of second order with four singularities. Duke Math. J. 9 (1), pp. 48–58.