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31: 3.6 Linear Difference Equations
Given numerical values of w 0 and w 1 , the solution w n of the equation …These errors have the effect of perturbing the solution by unwanted small multiples of w n and of an independent solution g n , say. … The unwanted multiples of g n now decay in comparison with w n , hence are of little consequence. … The latter method is usually superior when the true value of w 0 is zero or pathologically small. … beginning with e 0 = w 0 . …
32: 19.29 Reduction of General Elliptic Integrals
Let …where … Next, for j = 1 , 2 , define Q j ( t ) = f j + g j t + h j t 2 , and assume both Q ’s are positive for y < t < x . …where …If Q 1 ( t ) = ( a 1 + b 1 t ) ( a 2 + b 2 t ) , where both linear factors are positive for y < t < x , and Q 2 ( t ) = f 2 + g 2 t + h 2 t 2 , then (19.29.25) is modified so that …
33: Bibliography F
  • V. N. Faddeyeva and N. M. Terent’ev (1961) Tables of Values of the Function w ( z ) = e z 2 ( 1 + 2 i π 1 / 2 0 z e t 2 𝑑 t ) for Complex Argument. Edited by V. A. Fok; translated from the Russian by D. G. Fry. Mathematical Tables Series, Vol. 11, Pergamon Press, Oxford.
  • N. Fleury and A. Turbiner (1994) Polynomial relations in the Heisenberg algebra. J. Math. Phys. 35 (11), pp. 6144–6149.
  • A. S. Fokas and M. J. Ablowitz (1982) On a unified approach to transformations and elementary solutions of Painlevé equations. J. Math. Phys. 23 (11), pp. 2033–2042.
  • P. J. Forrester and N. S. Witte (2004) Application of the τ -function theory of Painlevé equations to random matrices: P VI , the JUE, CyUE, cJUE and scaled limits. Nagoya Math. J. 174, pp. 29–114.
  • L. W. Fullerton (1972) Algorithm 435: Modified incomplete gamma function. Comm. ACM 15 (11), pp. 993–995.
  • 34: 9.18 Tables
  • Harvard University (1945) tabulates the real and imaginary parts of h 1 ( z ) , h 1 ( z ) , h 2 ( z ) , h 2 ( z ) for x 0 z x 0 , 0 z y 0 , | x 0 + i y 0 | < 6.1 , with interval 0.1 in z and z . Precision is 8D. Here h 1 ( z ) = 2 4 / 3 3 1 / 6 i Ai ( e π i / 3 z ) , h 2 ( z ) = 2 4 / 3 3 1 / 6 i Ai ( e π i / 3 z ) .

  • Sherry (1959) tabulates a k , Ai ( a k ) , a k , Ai ( a k ) , k = 1 ( 1 ) 50 ; 20S.

  • National Bureau of Standards (1958) tabulates A 0 ( x ) π Hi ( x ) and A 0 ( x ) π Hi ( x ) for x = 0 ( .01 ) 1 ( .02 ) 5 ( .05 ) 11 and 1 / x = 0.01 ( .01 ) 0.1 ; 0 x A 0 ( t ) d t for x = 0.5 , 1 ( 1 ) 11 . Precision is 8D.

  • Nosova and Tumarkin (1965) tabulates e 0 ( x ) π Hi ( x ) , e 0 ( x ) = π Hi ( x ) , e ~ 0 ( x ) π Gi ( x ) , e ~ 0 ( x ) = π Gi ( x ) for x = 1 ( .01 ) 10 ; 7D. Also included are the real and imaginary parts of e 0 ( z ) and i e 0 ( z ) , where z = i y and y = 0 ( .01 ) 9 ; 6-7D.

  • Gil et al. (2003c) tabulates the only positive zero of Gi ( z ) , the first 10 negative real zeros of Gi ( z ) and Gi ( z ) , and the first 10 complex zeros of Gi ( z ) , Gi ( z ) , Hi ( z ) , and Hi ( z ) . Precision is 11 or 12S.

  • 35: 26.10 Integer Partitions: Other Restrictions
    p m ( 𝒟 , n ) denotes the number of partitions of n into at most m distinct parts. …The set { n 1 | n ± j ( mod k ) } is denoted by A j , k . … It is known that for k > 3 , p ( 𝒟 k , n ) p ( A 1 , k + 3 , n ) , with strict inequality for n sufficiently large, provided that k = 2 m 1 , m = 3 , 4 , 5 , or k 32 ; see Yee (2004). … where I 1 ( x ) is the modified Bessel function (§10.25(ii)), and …The quantity A k ( n ) is real-valued. …
    36: 24.12 Zeros
    For the interval 1 2 x < denote the zeros of B n ( x ) by x j ( n ) , j = 1 , 2 , , with … Let R ( n ) be the total number of real zeros of B n ( x ) . … For the interval 1 2 x < denote the zeros of E n ( x ) by y j ( n ) , j = 1 , 2 , , with … When n is odd y 1 ( n ) = 1 2 , … B n ( x ) , n = 1 , 2 , , has no multiple zeros. …
    37: Bibliography B
  • R. Barakat (1961) Evaluation of the incomplete gamma function of imaginary argument by Chebyshev polynomials. Math. Comp. 15 (73), pp. 7–11.
  • B. C. Berndt, S. Bhargava, and F. G. Garvan (1995) Ramanujan’s theories of elliptic functions to alternative bases. Trans. Amer. Math. Soc. 347 (11), pp. 4163–4244.
  • F. Bethuel (1998) Vortices in Ginzburg-Landau Equations. In Proceedings of the International Congress of Mathematicians, Vol. III (Berlin, 1998), pp. 11–19.
  • A. Bhattacharyya and L. Shafai (1988) Theoretical and experimental investigation of the elliptical annual ring antenna. IEEE Trans. Antennas and Propagation 36 (11), pp. 1526–1530.
  • R. L. Bishop (1981) Rainbow over Woolsthorpe Manor. Notes and Records Roy. Soc. London 36 (1), pp. 3–11 (1 plate).
  • 38: 5.10 Continued Fractions
    where
    a 0 = 1 12 ,
    a 1 = 1 30 ,
    a 2 = 53 210 ,
    For exact values of a 7 to a 11 and 40S values of a 0 to a 40 , see Char (1980). …
    39: 34.3 Basic Properties: 3 j Symbol
    When any one of j 1 , j 2 , j 3 is equal to 0 , 1 2 , or 1 , the 3 j symbol has a simple algebraic form. …For these and other results, and also cases in which any one of j 1 , j 2 , j 3 is 3 2 or 2 , see Edmonds (1974, pp. 125–127). … Even permutations of columns of a 3 j symbol leave it unchanged; odd permutations of columns produce a phase factor ( 1 ) j 1 + j 2 + j 3 , for example, … Similar conventions apply to all subsequent summations in this chapter.For the polynomials P l see §18.3, and for the function Y l , m see §14.30. …
    40: 28.8 Asymptotic Expansions for Large q
    Also let ξ = 2 h cos x and D m ( ξ ) = e ξ 2 / 4 𝐻𝑒 m ( ξ ) 18.3). …
    σ m 1 + s 2 3 h + 4 s 2 + 3 2 7 h 2 + 19 s 3 + 59 s 2 11 h 3 + ,
    28.8.11 P m ( x ) 1 + s 2 3 h cos 2 x + 1 h 2 ( s 4 + 86 s 2 + 105 2 11 cos 4 x s 4 + 22 s 2 + 57 2 11 cos 2 x ) + ,
    The approximations are expressed in terms of Whittaker functions W κ , μ ( z ) and M κ , μ ( z ) with μ = 1 4 ; compare §2.8(vi). … Subsequently the asymptotic solutions involving either elementary or Whittaker functions are identified in terms of the Floquet solutions me ν ( z , q ) 28.12(ii)) and modified Mathieu functions M ν ( j ) ( z , h ) 28.20(iii)). …