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expansions in Airy functions

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21: 18.24 Hahn Class: Asymptotic Approximations
This expansion is in terms of the parabolic cylinder function and its derivative. … This expansion is in terms of confluent hypergeometric functions. … Both expansions are in terms of parabolic cylinder functions. … Dunster (2001b) provides various asymptotic expansions for C n ( x ; a ) as n , in terms of elementary functions or in terms of Bessel functions. … This expansion is uniformly valid in any compact x -interval on the real line and is in terms of parabolic cylinder functions. …
22: 10.20 Uniform Asymptotic Expansions for Large Order
§10.20 Uniform Asymptotic Expansions for Large Order
uniformly for z ( 0 , ) in all cases, where Ai and Bi are the Airy functions9.2). …
§10.20(iii) Double Asymptotic Properties
For asymptotic properties of the expansions (10.20.4)–(10.20.6) with respect to large values of z see §10.41(v).
23: Bibliography V
  • O. Vallée and M. Soares (2010) Airy Functions and Applications to Physics. Second edition, Imperial College Press, London.
  • B. Ph. van Milligen and A. López Fraguas (1994) Expansion of vacuum magnetic fields in toroidal harmonics. Comput. Phys. Comm. 81 (1-2), pp. 74–90.
  • R. Vidūnas and N. M. Temme (2002) Symbolic evaluation of coefficients in Airy-type asymptotic expansions. J. Math. Anal. Appl. 269 (1), pp. 317–331.
  • H. Volkmer (1999) Expansions in products of Heine-Stieltjes polynomials. Constr. Approx. 15 (4), pp. 467–480.
  • H. Volkmer and J. J. Wood (2014) A note on the asymptotic expansion of generalized hypergeometric functions. Anal. Appl. (Singap.) 12 (1), pp. 107–115.
  • 24: 10.21 Zeros
    §10.21(vi) McMahon’s Asymptotic Expansions for Large Zeros
    §10.21(vii) Asymptotic Expansions for Large Order
    Let 𝒞 ν ( x ) , ρ ν ( t ) , and σ ν ( t ) be defined as in §10.21(ii) and M ( x ) , θ ( x ) , N ( x ) , and ϕ ( x ) denote the modulus and phase functions for the Airy functions and their derivatives as in §9.8. … Here a m and a m denote respectively the zeros of the Airy function Ai ( z ) and its derivative Ai ( z ) ; see §9.9. … Higher coefficients in the asymptotic expansions in this subsection can be obtained by expressing the cross-products in terms of the modulus and phase functions10.18), and then reverting the asymptotic expansion for the difference of the phase functions. …
    25: 2.2 Transcendental Equations
    An important case is the reversion of asymptotic expansions for zeros of special functions. In place of (2.2.1) assume that …where F 0 = f 0 and s F s ( s 1 ) is the coefficient of x 1 in the asymptotic expansion of ( f ( x ) ) s (Lagrange’s formula for the reversion of series). Conditions for the validity of the reversion process in are derived in Olver (1997b, pp. 14–16). Applications to real and complex zeros of Airy functions are given in Fabijonas and Olver (1999). …
    26: 9.13 Generalized Airy Functions
    §9.13 Generalized Airy Functions
    The distribution in and asymptotic properties of the zeros of A n ( z ) , A n ( z ) , B n ( z ) , and B n ( z ) are investigated in Swanson and Headley (1967) and Headley and Barwell (1975). … Reid (1972) and Drazin and Reid (1981, Appendix) introduce the following contour integrals in constructing approximate solutions to the Orr–Sommerfeld equation for fluid flow: …
    27: 10.19 Asymptotic Expansions for Large Order
    §10.19 Asymptotic Expansions for Large Order
    §10.19(i) Asymptotic Forms
    §10.19(ii) Debye’s Expansions
    Here Ai and Bi are the Airy functions9.2), and … See also §10.20(i).
    28: 12.11 Zeros
    §12.11(ii) Asymptotic Expansions of Large Zeros
    §12.11(iii) Asymptotic Expansions for Large Parameter
    For large negative values of a the real zeros of U ( a , x ) , U ( a , x ) , V ( a , x ) , and V ( a , x ) can be approximated by reversion of the Airy-type asymptotic expansions of §§12.10(vii) and 12.10(viii). …Here α = μ 4 3 a s , a s denoting the s th negative zero of the function Ai (see §9.9(i)). … where β = μ 4 3 a s , a s denoting the s th negative zero of the function Ai and …
    29: 9.9 Zeros
    They are denoted by a k , a k , b k , b k , respectively, arranged in ascending order of absolute value for k = 1 , 2 , .
    §9.9(ii) Relation to Modulus and Phase
    §9.9(iv) Asymptotic Expansions
    For error bounds for the asymptotic expansions of a k , b k , a k , and b k see Pittaluga and Sacripante (1991), and a conjecture given in Fabijonas and Olver (1999).
    §9.9(v) Tables
    30: 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.
  • E. Jahnke and F. Emde (1945) Tables of Functions with Formulae and Curves. 4th edition, Dover Publications, New York.
  • U. D. Jentschura and E. Lötstedt (2012) Numerical calculation of Bessel, Hankel and Airy functions. Computer Physics Communications 183 (3), pp. 506–519.
  • 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.
  • W. B. Jones and W. Van Assche (1998) Asymptotic behavior of the continued fraction coefficients of a class of Stieltjes transforms including the Binet function. In Orthogonal functions, moment theory, and continued fractions (Campinas, 1996), Lecture Notes in Pure and Appl. Math., Vol. 199, pp. 257–274.