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21: 24.19 Methods of Computation
If N ~ 2 n denotes the right-hand side of (24.19.1) but with the second product taken only for p ( π e ) 1 2 n + 1 , then N 2 n = N ~ 2 n for n 2 . … For other information see Chellali (1988) and Zhang and Jin (1996, pp. 1–11). For algorithms for computing B n , E n , B n ( x ) , and E n ( x ) see Spanier and Oldham (1987, pp. 37, 41, 171, and 179–180). … For number-theoretic applications it is important to compute B 2 n ( mod p ) for 2 n p 3 ; in particular to find the irregular pairs ( 2 n , p ) for which B 2 n 0 ( mod p ) . …
  • Buhler et al. (1992) uses the expansion

    24.19.3 t 2 cosh t 1 = 2 n = 0 ( 2 n 1 ) B 2 n t 2 n ( 2 n ) ! ,

    and computes inverses modulo p of the left-hand side. Multisectioning techniques are applied in implementations. See also Crandall (1996, pp. 116–120).

  • 22: Bibliography E
  • C. Eckart (1930) The penetration of a potential barrier by electrons. Phys. Rev. 35 (11), pp. 1303–1309.
  • F. H. L. Essler, H. Frahm, A. R. Its, and V. E. Korepin (1996) Painlevé transcendent describes quantum correlation function of the X X Z antiferromagnet away from the free-fermion point. J. Phys. A 29 (17), pp. 5619–5626.
  • L. Euler (1768) Institutiones Calculi Integralis. Opera Omnia (1), Vol. 11, pp. 110–113.
  • W. N. Everitt, L. L. Littlejohn, and R. Wellman (2004) The Sobolev orthogonality and spectral analysis of the Laguerre polynomials { L n k } for positive integers k . J. Comput. Appl. Math. 171 (1-2), pp. 199–234.
  • W. N. Everitt (2008) Note on the X 1 -Laguerre orthogonal polynomials.
  • 23: Bibliography K
  • E. L. Kaplan (1948) Auxiliary table for the incomplete elliptic integrals. J. Math. Physics 27, pp. 11–36.
  • S. K. Kim (1972) The asymptotic expansion of a hypergeometric function F 2 2 ( 1 , α ; ρ 1 , ρ 2 ; z ) . Math. Comp. 26 (120), pp. 963.
  • Y. S. Kim, A. K. Rathie, and R. B. Paris (2013) An extension of Saalschütz’s summation theorem for the series F r + 2 r + 3 . Integral Transforms Spec. Funct. 24 (11), pp. 916–921.
  • K. S. Kölbig (1968) Algorithm 327: Dilogarithm [S22]. Comm. ACM 11 (4), pp. 270–271.
  • T. H. Koornwinder (1981) Clebsch-Gordan coefficients for SU ( 2 ) and Hahn polynomials. Nieuw Arch. Wisk. (3) 29 (2), pp. 140–155.
  • 24: Bibliography L
  • A. Leitner and J. Meixner (1960) Eine Verallgemeinerung der Sphäroidfunktionen. Arch. Math. 11, pp. 29–39.
  • M. Lerch (1887) Note sur la fonction 𝔎 ( w , x , s ) = k = 0 e 2 k π i x ( w + k ) s . Acta Math. 11 (1-4), pp. 19–24 (French).
  • H. Lotsch and M. Gray (1964) Algorithm 244: Fresnel integrals. Comm. ACM 7 (11), pp. 660–661.
  • N. A. Lukaševič (1967b) On the theory of Painlevé’s third equation. Differ. Uravn. 3 (11), pp. 1913–1923 (Russian).
  • Y. L. Luke (1977a) Algorithms for rational approximations for a confluent hypergeometric function. Utilitas Math. 11, pp. 123–151.
  • 25: Bibliography H
  • L. Habsieger (1986) La q -conjecture de Macdonald-Morris pour G 2 . C. R. Acad. Sci. Paris Sér. I Math. 303 (6), pp. 211–213 (French).
  • R. S. Heller (1976) 25D Table of the First One Hundred Values of j 0 , s , J 1 ( j 0 , s ) , j 1 , s , J 0 ( j 1 , s ) = J 0 ( j 0 , s + 1 ) , j 1 , s , J 1 ( j 1 , s ) . Technical report Department of Physics, Worcester Polytechnic Institute, Worcester, MA.
  • D. R. Herrick and S. O’Connor (1998) Inverse virial symmetry of diatomic potential curves. J. Chem. Phys. 109 (1), pp. 11–19.
  • G. W. Hill (1970) Algorithm 395: Student’s t-distribution. Comm. ACM 13 (10), pp. 617–619.
  • G. W. Hill (1981) Algorithm 571: Statistics for von Mises’ and Fisher’s distributions of directions: I 1 ( x ) / I 0 ( x ) , I 1.5 ( x ) / I 0.5 ( x ) and their inverses [S14]. ACM Trans. Math. Software 7 (2), pp. 233–238.
  • 26: Bibliography O
  • K. Okamoto (1986) Studies on the Painlevé equations. III. Second and fourth Painlevé equations, P II and P IV . Math. Ann. 275 (2), pp. 221–255.
  • M. N. Olevskiĭ (1950) Triorthogonal systems in spaces of constant curvature in which the equation Δ 2 u + λ u = 0 allows a complete separation of variables. Mat. Sbornik N.S. 27(69) (3), pp. 379–426 (Russian).
  • F. W. J. Olver (1974) Error bounds for stationary phase approximations. SIAM J. Math. Anal. 5 (1), pp. 19–29.
  • S. Olver (2011) Numerical solution of Riemann-Hilbert problems: Painlevé II. Found. Comput. Math. 11 (2), pp. 153–179.
  • H. Oser (1960) Algorithm 22: Riccati-Bessel functions of first and second kind. Comm. ACM 3 (11), pp. 600–601.
  • 27: 34.5 Basic Properties: 6 j Symbol
    If any lower argument in a 6 j symbol is 0 , 1 2 , or 1 , then the 6 j symbol has a simple algebraic form. …
    34.5.9 { j 1 j 2 j 3 l 1 l 2 l 3 } = { j 1 1 2 ( j 2 + l 2 + j 3 l 3 ) 1 2 ( j 2 l 2 + j 3 + l 3 ) l 1 1 2 ( j 2 + l 2 j 3 + l 3 ) 1 2 ( j 2 + l 2 + j 3 + l 3 ) } ,
    34.5.11 ( 2 j 1 + 1 ) ( ( J 3 + J 2 J 1 ) ( L 3 + L 2 J 1 ) 2 ( J 3 L 3 + J 2 L 2 J 1 L 1 ) ) { j 1 j 2 j 3 l 1 l 2 l 3 } = j 1 E ( j 1 + 1 ) { j 1 + 1 j 2 j 3 l 1 l 2 l 3 } + ( j 1 + 1 ) E ( j 1 ) { j 1 1 j 2 j 3 l 1 l 2 l 3 } ,
    34.5.16 ( 1 ) j 1 + j 2 + j 3 + j 1 + j 2 + l 1 + l 2 { j 1 j 2 j 3 l 1 l 2 l 3 } { j 1 j 2 j 3 l 1 l 2 l 3 } = j ( 1 ) l 3 + l 3 + j ( 2 j + 1 ) { j 1 j 1 j j 2 j 2 j 3 } { l 3 l 3 j j 1 j 1 l 2 } { l 3 l 3 j j 2 j 2 l 1 } .
    34.5.23 ( j 1 j 2 j 3 m 1 m 2 m 3 ) { j 1 j 2 j 3 l 1 l 2 l 3 } = m 1 m 2 m 3 ( 1 ) l 1 + l 2 + l 3 + m 1 + m 2 + m 3 ( j 1 l 2 l 3 m 1 m 2 m 3 ) ( l 1 j 2 l 3 m 1 m 2 m 3 ) ( l 1 l 2 j 3 m 1 m 2 m 3 ) .
    28: Bibliography D
  • D. Dominici, S. J. Johnston, and K. Jordaan (2013) Real zeros of F 1 2 hypergeometric polynomials. J. Comput. Appl. Math. 247, pp. 152–161.
  • E. Dorrer (1968) Algorithm 322. F-distribution. Comm. ACM 11 (2), pp. 116–117.
  • B. A. Dubrovin (1981) Theta functions and non-linear equations. Uspekhi Mat. Nauk 36 (2(218)), pp. 11–80 (Russian).
  • T. M. Dunster (2003a) Uniform asymptotic approximations for the Whittaker functions M κ , i μ ( z ) and W κ , i μ ( z ) . Anal. Appl. (Singap.) 1 (2), pp. 199–212.
  • J. Dutka (1981) The incomplete beta function—a historical profile. Arch. Hist. Exact Sci. 24 (1), pp. 1129.
  • 29: 11.14 Tables
  • Abramowitz and Stegun (1964, Chapter 12) tabulates 𝐇 n ( x ) , 𝐇 n ( x ) Y n ( x ) , and I n ( x ) 𝐋 n ( x ) for n = 0 , 1 and x = 0 ( .1 ) 5 , x 1 = 0 ( .01 ) 0.2 to 6D or 7D.

  • Abramowitz and Stegun (1964, Chapter 12) tabulates 0 x ( I 0 ( t ) 𝐋 0 ( t ) ) d t and ( 2 / π ) x t 1 𝐇 0 ( t ) d t for x = 0 ( .1 ) 5 to 5D or 7D; 0 x ( 𝐇 0 ( t ) Y 0 ( t ) ) d t ( 2 / π ) ln x , 0 x ( I 0 ( t ) 𝐋 0 ( t ) ) d t ( 2 / π ) ln x , and x t 1 ( 𝐇 0 ( t ) Y 0 ( t ) ) d t for x 1 = 0 ( .01 ) 0.2 to 6D.

  • Agrest et al. (1982) tabulates 0 x 𝐇 0 ( t ) d t and e x 0 x 𝐋 0 ( t ) d t for x = 0 ( .001 ) 5 ( .005 ) 15 ( .01 ) 100 to 11D.

  • Jahnke and Emde (1945) tabulates 𝐄 n ( x ) for n = 1 , 2 and x = 0 ( .01 ) 14.99 to 4D.

  • Agrest and Maksimov (1971, Chapter 11) defines incomplete Struve, Anger, and Weber functions and includes tables of an incomplete Struve function 𝐇 n ( x , α ) for n = 0 , 1 , x = 0 ( .2 ) 10 , and α = 0 ( .2 ) 1.4 , 1 2 π , together with surface plots.

  • 30: 3.7 Ordinary Differential Equations
    The path is partitioned at P + 1 points labeled successively z 0 , z 1 , , z P , with z 0 = a , z P = b . … Let 𝐀 P be the ( 2 P ) × ( 2 P + 2 ) band matrix … This is a set of 2 P equations for the 2 P + 2 unknowns, w ( z j ) and w ( z j ) , j = 0 , 1 , , P . … The values λ k are the eigenvalues and the corresponding solutions w k of the differential equation are the eigenfunctions. … where h = z n + 1 z n and …