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艾里森山大学商业管理文凭证书【somewhat微aptao168】1949a

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11: Bibliography G
  • J. A. Gaunt (1929) The triplets of helium. Philos. Trans. Roy. Soc. London Ser. A 228, pp. 151–196.
  • A. Gil and J. Segura (2001) DTORH3 2.0: A new version of a computer program for the evaluation of toroidal harmonics. Comput. Phys. Comm. 139 (2), pp. 186–191.
  • W. Gröbner and N. Hofreiter (1949) Integraltafel. Erster Teil. Unbestimmte Integrale. Springer-Verlag, Vienna.
  • H. Gupta (1935) A table of partitions. Proc. London Math. Soc. (2) 39, pp. 142–149.
  • H. Gupta (1937) A table of partitions (II). Proc. London Math. Soc. (2) 42, pp. 546–549.
  • 12: Bibliography
  • M. Abramowitz (1949) Asymptotic expansions of spheroidal wave functions. J. Math. Phys. Mass. Inst. Tech. 28, pp. 195–199.
  • C. L. Adler, J. A. Lock, B. R. Stone, and C. J. Garcia (1997) High-order interior caustics produced in scattering of a diagonally incident plane wave by a circular cylinder. J. Opt. Soc. Amer. A 14 (6), pp. 1305–1315.
  • G. B. Airy (1838) On the intensity of light in the neighbourhood of a caustic. Trans. Camb. Phil. Soc. 6, pp. 379–402.
  • G. B. Airy (1849) Supplement to a paper “On the intensity of light in the neighbourhood of a caustic”. Trans. Camb. Phil. Soc. 8, pp. 595–599.
  • D. E. Amos (1985) A subroutine package for Bessel functions of a complex argument and nonnegative order. Technical Report Technical Report SAND85-1018, Sandia National Laboratories, Albuquerque, NM.
  • 13: 30.9 Asymptotic Approximations and Expansions
    The asymptotic behavior of λ n m ( γ 2 ) and a n , k m ( γ 2 ) as n in descending powers of 2 n + 1 is derived in Meixner (1944). The cases of large m , and of large m and large | γ | , are studied in Abramowitz (1949). …
    14: 4.26 Integrals
    4.26.7 e a x sin ( b x ) d x = e a x a 2 + b 2 ( a sin ( b x ) b cos ( b x ) ) ,
    4.26.8 e a x cos ( b x ) d x = e a x a 2 + b 2 ( a cos ( b x ) + b sin ( b x ) ) .
    4.26.9 0 π sin ( m t ) sin ( n t ) d t = 0 , m n ,
    4.26.10 0 π cos ( m t ) cos ( n t ) d t = 0 , m n ,
    Extensive compendia of indefinite and definite integrals of trigonometric and inverse trigonometric functions include Apelblat (1983, pp. 48–109), Bierens de Haan (1939), Gradshteyn and Ryzhik (2000, Chapters 2–4), Gröbner and Hofreiter (1949, pp. 116–139), Gröbner and Hofreiter (1950, pp. 94–160), and Prudnikov et al. (1986a, §§1.5, 1.7, 2.5, 2.7).
    15: 1.15 Summability Methods
    (Here and elsewhere in this subsection δ is a constant such that 0 < δ < π .) … A ( r , θ ) is a harmonic function in polar coordinates (1.9.27), and … The lower limit 0 of the integral in (1.15.47) can be replaced by any constant a x . Also, we can replace the lower and upper limits of the integral by x and a , respectively. … and either | a n | K or a n 0 , then …
    16: 18.16 Zeros
    where a m is the m th negative zero of Ai ( x ) 9.9(i)). …
    18.16.15 x n , m < ν + 2 2 3 a m ν 1 3 + 2 2 3 a m 2 ν 1 3 ,
    18.16.17 x n , m = ( 2 n + 1 ) 1 2 + 2 1 3 ( 2 n + 1 ) 1 6 a m + ϵ n , m ,
    where a m is the m th negative zero of Ai ( x ) 9.9(i)), ϵ n , m < 0 , and as n with m fixed … In the notation of this reference x n , m = u a , m , μ = 2 n + 1 , and α = μ 4 3 a m . …
    17: 1.4 Calculus of One Variable
    For extensive tables of integrals, see Apelblat (1983), Bierens de Haan (1867), Gradshteyn and Ryzhik (2000), Gröbner and Hofreiter (1949, 1950), and Prudnikov et al. (1986a, b, 1990, 1992a, 1992b). … A function f ( x ) is square-integrable if … With a < b , the total variation of f ( x ) on a finite or infinite interval ( a , b ) is … A function f ( x ) is convex on ( a , b ) if …A similar definition applies to closed intervals [ a , b ] . …
    18: Bibliography M
  • T. Masuda, Y. Ohta, and K. Kajiwara (2002) A determinant formula for a class of rational solutions of Painlevé V equation. Nagoya Math. J. 168, pp. 1–25.
  • J. Meixner (1944) Die Laméschen Wellenfunktionen des Drehellipsoids. Forschungsbericht No. 1952 ZWB (German).
  • A. Michaeli (1996) Asymptotic analysis of edge-excited currents on a convex face of a perfectly conducting wedge under overlapping penumbra region conditions. IEEE Trans. Antennas and Propagation 44 (1), pp. 97–101.
  • MuPAD (commercial interactive system and Matlab toolbox) SciFace Software, Paderborn, Germany.
  • L. A. Muraveĭ (1976) Zeros of the function A i ( z ) σ A i ( z ) . Differential Equations 11, pp. 797–811.
  • 19: 28.8 Asymptotic Expansions for Large q
    These results are derived formally in Sips (1949, 1959, 1965). … Let x = 1 2 π μ h 1 / 4 , where μ is a constant such that μ 1 , and s = 2 m + 1 . … The approximations apply when the parameters a and q are real and large, and are uniform with respect to various regions in the z -plane. … These approximations apply when q and a are real and q . They are uniform with respect to a when 2 q a ( 2 δ ) q , where δ is an arbitrary constant such that 0 < δ < 4 , and also with respect to z in the semi-infinite strip given by 0 z π and z 0 . …
    20: Bibliography S
  • J. Segura (1998) A global Newton method for the zeros of cylinder functions. Numer. Algorithms 18 (3-4), pp. 259–276.
  • J. Shao and P. Hänggi (1998) Decoherent dynamics of a two-level system coupled to a sea of spins. Phys. Rev. Lett. 81 (26), pp. 5710–5713.
  • A. Sidi (2003) Practical Extrapolation Methods: Theory and Applications. Cambridge Monographs on Applied and Computational Mathematics, Vol. 10, Cambridge University Press, Cambridge.
  • R. Sips (1949) Représentation asymptotique des fonctions de Mathieu et des fonctions d’onde sphéroidales. Trans. Amer. Math. Soc. 66 (1), pp. 93–134 (French).
  • A. N. Stokes (1980) A stable quotient-difference algorithm. Math. Comp. 34 (150), pp. 515–519.