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21: 29.7 Asymptotic Expansions
29.7.3 τ 0 = 1 2 3 ( 1 + k 2 ) ( 1 + p 2 ) ,
29.7.4 τ 1 = p 2 6 ( ( 1 + k 2 ) 2 ( p 2 + 3 ) 4 k 2 ( p 2 + 5 ) ) .
29.7.6 τ 2 = 1 2 10 ( 1 + k 2 ) ( 1 k 2 ) 2 ( 5 p 4 + 34 p 2 + 9 ) ,
29.7.7 τ 3 = p 2 14 ( ( 1 + k 2 ) 4 ( 33 p 4 + 410 p 2 + 405 ) 24 k 2 ( 1 + k 2 ) 2 ( 7 p 4 + 90 p 2 + 95 ) + 16 k 4 ( 9 p 4 + 130 p 2 + 173 ) ) ,
29.7.8 τ 4 = 1 2 16 ( ( 1 + k 2 ) 5 ( 63 p 6 + 1260 p 4 + 2943 p 2 + 486 ) 8 k 2 ( 1 + k 2 ) 3 ( 49 p 6 + 1010 p 4 + 2493 p 2 + 432 ) + 16 k 4 ( 1 + k 2 ) ( 35 p 6 + 760 p 4 + 2043 p 2 + 378 ) ) .
22: Bibliography N
  • G. Nemes (2013c) Generalization of Binet’s Gamma function formulas. Integral Transforms Spec. Funct. 24 (8), pp. 597–606.
  • N. Nielsen (1909) Der Eulersche Dilogarithmus und seine Verallgemeinerungen. Nova Acta Leopoldina 90, pp. 123–212.
  • V. Yu. Novokshënov (1985) The asymptotic behavior of the general real solution of the third Painlevé equation. Dokl. Akad. Nauk SSSR 283 (5), pp. 1161–1165 (Russian).
  • Numerical Recipes (commercial C, C++, Fortran 77, and Fortran 90 libraries)
  • H. M. Nussenzveig (1965) High-frequency scattering by an impenetrable sphere. Ann. Physics 34 (1), pp. 23–95.
  • 23: 35.2 Laplace Transform
    Suppose there exists a constant 𝐗 0 𝛀 such that | f ( 𝐗 ) | < etr ( 𝐗 0 𝐗 ) for all 𝐗 𝛀 . Then (35.2.1) converges absolutely on the region ( 𝐙 ) > 𝐗 0 , and g ( 𝐙 ) is a complex analytic function of all elements z j , k of 𝐙 . … Assume that 𝓢 | g ( 𝐔 + i 𝐕 ) | d 𝐕 converges, and also that its limit as 𝐔 is 0 . …where the integral is taken over all 𝐙 = 𝐔 + i 𝐕 such that 𝐔 > 𝐗 0 and 𝐕 ranges over 𝓢 . … If g j is the Laplace transform of f j , j = 1 , 2 , then g 1 g 2 is the Laplace transform of the convolution f 1 f 2 , where …
    24: 20.4 Values at z = 0
    20.4.1 θ 1 ( 0 , q ) = θ 2 ( 0 , q ) = θ 3 ( 0 , q ) = θ 4 ( 0 , q ) = 0 ,
    20.4.2 θ 1 ( 0 , q ) = 2 q 1 / 4 n = 1 ( 1 q 2 n ) 3 = 2 q 1 / 4 ( q 2 ; q 2 ) 3 ,
    20.4.9 θ 2 ′′ ( 0 , q ) θ 2 ( 0 , q ) = 1 8 n = 1 q 2 n ( 1 + q 2 n ) 2 ,
    20.4.10 θ 3 ′′ ( 0 , q ) θ 3 ( 0 , q ) = 8 n = 1 q 2 n 1 ( 1 + q 2 n 1 ) 2 ,
    20.4.11 θ 4 ′′ ( 0 , q ) θ 4 ( 0 , q ) = 8 n = 1 q 2 n 1 ( 1 q 2 n 1 ) 2 .
    25: 4.10 Integrals
    Extensive compendia of indefinite and definite integrals of logarithms and exponentials include Apelblat (1983, pp. 16–47), Bierens de Haan (1939), Gröbner and Hofreiter (1949, pp. 107–116), Gröbner and Hofreiter (1950, pp. 52–90), Gradshteyn and Ryzhik (2000, Chapters 2–4), and Prudnikov et al. (1986a, §§1.3, 1.6, 2.3, 2.6).
    26: Bibliography T
  • I. C. Tang (1969) Some definite integrals and Fourier series for Jacobian elliptic functions. Z. Angew. Math. Mech. 49, pp. 9596.
  • N. M. Temme (1994a) A set of algorithms for the incomplete gamma functions. Probab. Engrg. Inform. Sci. 8, pp. 291–307.
  • N. M. Temme (1995b) Bernoulli polynomials old and new: Generalizations and asymptotics. CWI Quarterly 8 (1), pp. 47–66.
  • P. Terwilliger (2013) The universal Askey-Wilson algebra and DAHA of type ( C 1 , C 1 ) . SIGMA 9, pp. Paper 047, 40 pp..
  • W. J. Thompson (1997) Atlas for Computing Mathematical Functions: An Illustrated Guide for Practitioners. John Wiley & Sons Inc., New York.
  • 27: 26.6 Other Lattice Path Numbers
    Delannoy Number D ( m , n )
    D ( m , n ) is the number of paths from ( 0 , 0 ) to ( m , n ) that are composed of directed line segments of the form ( 1 , 0 ) , ( 0 , 1 ) , or ( 1 , 1 ) . …
    26.6.12 C ( n ) = k = 1 n N ( n , k ) ,
    26.6.13 M ( n ) = k = 0 n ( 1 ) k ( n k ) C ( n + 1 k ) ,
    26.6.14 C ( n ) = k = 0 2 n ( 1 ) k ( 2 n k ) M ( 2 n k ) .
    28: Bibliography G
  • G. Gasper and M. Rahman (1990) Basic Hypergeometric Series. Encyclopedia of Mathematics and its Applications, Vol. 35, Cambridge University Press, Cambridge.
  • G. Gasper and M. Rahman (2004) Basic Hypergeometric Series. Second edition, Encyclopedia of Mathematics and its Applications, Vol. 96, Cambridge University Press, Cambridge.
  • W. Gautschi (1964b) Algorithm 236: Bessel functions of the first kind. Comm. ACM 7 (8), pp. 479–480.
  • W. Gautschi (1965) Algorithm 259: Legendre functions for arguments larger than one. Comm. ACM 8 (8), pp. 488–492.
  • A. Gil, J. Segura, and N. M. Temme (2012) An improved algorithm and a Fortran 90 module for computing the conical function P 1 / 2 + i τ m ( x ) . Comput. Phys. Commun. 183 (3), pp. 794–799.
  • 29: 25.6 Integer Arguments
    ζ ( 4 ) = π 4 90 ,
    25.6.2 ζ ( 2 n ) = ( 2 π ) 2 n 2 ( 2 n ) ! | B 2 n | , n = 1 , 2 , 3 , .
    25.6.3 ζ ( n ) = B n + 1 n + 1 , n = 1 , 2 , 3 , .
    25.6.4 ζ ( 2 n ) = 0 , n = 1 , 2 , 3 , .
    With c defined by (25.4.6) and n = 1 , 2 , 3 , , …
    30: 4.5 Inequalities
    4.5.3 | ln ( 1 x ) | < 3 2 x , 0 < x 0.5828 ,
    For more inequalities involving the exponential function see Mitrinović (1964, pp. 73–77), Mitrinović (1970, pp. 266–271), and Bullen (1998, pp. 81–83).