About the Project

%E7%BD%91%E4%B8%8A%E5%8D%9A%E5%BD%A9%E5%B9%B3%E5%8F%B0,%E4%BA%9A%E6%B4%B2%E5%8D%9A%E5%BD%A9%E5%B9%B3%E5%8F%B0%E6%8E%A8%E8%8D%90,%E7%BA%BF%E4%B8%8A%E5%8D%9A%E5%BD%A9%E5%85%AC%E5%8F%B8,%E3%80%90%E5%8D%9A%E5%BD%A9%E6%B8%B8%E6%88%8F%E5%9C%B0%E5%9D%80%E2%88%B633kk66.com%E3%80%91%E7%AB%9E%E5%8D%9A%E5%BD%A9%E5%B9%B3%E5%8F%B0,%E4%BA%9A%E6%B4%B2%E5%8D%9A%E5%BD%A9%E5%B9%B3%E5%8F%B0,%E5%9C%A8%E7%BA%BF%E5%8D%9A%E5%BD%A9%E5%B9%B3%E5%8F%B0%E7%BD%91%E5%9D%80%E5%A4%A7%E5%85%A8,%E8%8F%B2%E5%BE%8B%E5%AE%BE%E5%8D%9A%E5%BD%A9%E7%BD%91%E5%9D%80,%E6%94%AF%E6%8C%81%E4%BA%BA%E6%B0%91%E5%B8%81%E7%9A%84%E5%8D%9A%E5%BD%A9%E5%85%AC%E5%8F%B8,%E3%80%90%E5%8D%9A%E5%BD%A9%E5%B9%B3%E5%8F%B0%E2%88%B633kk66.com%E3%80%91

AdvancedHelp

(0.082 seconds)

21—30 of 757 matching pages

21: Bibliography K
  • W. Kahan (1987) Branch Cuts for Complex Elementary Functions or Much Ado About Nothing’s Sign Bit. In The State of the Art in Numerical Analysis (Birmingham, 1986), A. Iserles and M. J. D. Powell (Eds.), Inst. Math. Appl. Conf. Ser. New Ser., Vol. 9, pp. 165–211.
  • K. Kajiwara and Y. Ohta (1996) Determinant structure of the rational solutions for the Painlevé II equation. J. Math. Phys. 37 (9), pp. 4693–4704.
  • M. Kaneko (1997) Poly-Bernoulli numbers. J. Théor. Nombres Bordeaux 9 (1), pp. 221–228.
  • M. K. Kerimov (2008) Overview of some new results concerning the theory and applications of the Rayleigh special function. Comput. Math. Math. Phys. 48 (9), pp. 1454–1507.
  • E. Kreyszig (1957) On the zeros of the Fresnel integrals. Canad. J. Math. 9, pp. 118–131.
  • 22: 16.24 Physical Applications
    §16.24(iii) 3 j , 6 j , and 9 j Symbols
    They can be expressed as F 2 3 functions with unit argument. …These are balanced F 3 4 functions with unit argument. Lastly, special cases of the 9 j symbols are F 4 5 functions with unit argument. …
    23: 19.36 Methods of Computation
    If (19.36.1) is used instead of its first five terms, then the factor ( 3 r ) 1 / 6 in Carlson (1995, (2.2)) is changed to ( 3 r ) 1 / 8 . For both R D and R J the factor ( r / 4 ) 1 / 6 in Carlson (1995, (2.18)) is changed to ( r / 5 ) 1 / 8 when the following polynomial of degree 7 (the same for both) is used instead of its first seven terms: … All cases of R F , R C , R J , and R D are computed by essentially the same procedure (after transforming Cauchy principal values by means of (19.20.14) and (19.2.20)). … The incomplete integrals R F ( x , y , z ) and R G ( x , y , z ) can be computed by successive transformations in which two of the three variables converge quadratically to a common value and the integrals reduce to R C , accompanied by two quadratically convergent series in the case of R G ; compare Carlson (1965, §§5,6). … F ( ϕ , k ) can be evaluated by using (19.25.5). …
    24: 18.8 Differential Equations
    Table 18.8.1: Classical OP’s: differential equations A ( x ) f ′′ ( x ) + B ( x ) f ( x ) + C ( x ) f ( x ) + λ n f ( x ) = 0 .
    # f ( x ) A ( x ) B ( x ) C ( x ) λ n
    4 C n ( λ ) ( x ) 1 x 2 ( 2 λ + 1 ) x 0 n ( n + 2 λ )
    8 L n ( α ) ( x ) x α + 1 x 0 n
    9 e 1 2 x 2 x α + 1 2 L n ( α ) ( x 2 ) 1 0 x 2 + ( 1 4 α 2 ) x 2 4 n + 2 α + 2
    25: Bibliography D
  • S. D. Daymond (1955) The principal frequencies of vibrating systems with elliptic boundaries. Quart. J. Mech. Appl. Math. 8 (3), pp. 361–372.
  • G. Doetsch (1955) Handbuch der Laplace-Transformation. Bd. II. Anwendungen der Laplace-Transformation. 1. Abteilung. Birkhäuser Verlag, Basel und Stuttgart (German).
  • K. Driver and K. Jordaan (2013) Inequalities for extreme zeros of some classical orthogonal and q -orthogonal polynomials. Math. Model. Nat. Phenom. 8 (1), pp. 48–59.
  • G. V. Dunne and K. Rao (2000) Lamé instantons. J. High Energy Phys. 2000 (1), pp. Paper 19, 8.
  • L. Durand (1978) Product formulas and Nicholson-type integrals for Jacobi functions. I. Summary of results. SIAM J. Math. Anal. 9 (1), pp. 76–86.
  • 26: 3.2 Linear Algebra
    Assume that 𝐀 can be factored as in (3.2.5), but without partial pivoting. … is called the characteristic polynomial of 𝐀 and its zeros are the eigenvalues of 𝐀 . … Let 𝐀 be an n × n symmetric matrix. …has the same eigenvalues as 𝐀 . … Many methods are available for computing eigenvalues; see Golub and Van Loan (1996, Chapters 7, 8), Trefethen and Bau (1997, Chapter 5), and Wilkinson (1988, Chapters 8, 9).
    27: 34.9 Graphical Method
    §34.9 Graphical Method
    Thus, any analytic expression in the theory, for example equations (34.3.16), (34.4.1), (34.5.15), and (34.7.3), may be represented by a diagram; conversely, any diagram represents an analytic equation. …For specific examples of the graphical method of representing sums involving the 3 j , 6 j , and 9 j symbols, see Varshalovich et al. (1988, Chapters 11, 12) and Lehman and O’Connell (1973, §3.3).
    28: 16.26 Approximations
    For discussions of the approximation of generalized hypergeometric functions and the Meijer G -function in terms of polynomials, rational functions, and Chebyshev polynomials see Luke (1975, §§5.12 - 5.13) and Luke (1977b, Chapters 1 and 9).
    29: 34.10 Zeros
    Such zeros are called nontrivial zeros. For further information, including examples of nontrivial zeros and extensions to 9 j symbols, see Srinivasa Rao and Rajeswari (1993, pp. 133–215, 294–295, 299–310).
    30: 34.13 Methods of Computation
    Methods of computation for 3 j and 6 j symbols include recursion relations, see Schulten and Gordon (1975a), Luscombe and Luban (1998), and Edmonds (1974, pp. 42–45, 48–51, 97–99); summation of single-sum expressions for these symbols, see Varshalovich et al. (1988, §§8.2.6, 9.2.1) and Fang and Shriner (1992); evaluation of the generalized hypergeometric functions of unit argument that represent these symbols, see Srinivasa Rao and Venkatesh (1978) and Srinivasa Rao (1981). For 9 j symbols, methods include evaluation of the single-sum series (34.6.2), see Fang and Shriner (1992); evaluation of triple-sum series, see Varshalovich et al. (1988, §10.2.1) and Srinivasa Rao et al. (1989). …