About the Project

.卡塔尔世界杯奖金_『网址:687.vii』世界杯竞猜_b5p6v3_2022年11月30日21时49分53秒_3vjzhlfvb.cc

AdvancedHelp

The terms "vjzhlfvb.cc", "b5p6v3" were not found.Possible alternative term: "primzahlfunct".

(0.005 seconds)

1—10 of 231 matching pages

1: 34.9 Graphical Method
For an account of this method see Brink and Satchler (1993, Chapter VII). 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).
2: Bibliography
  • W. A. Al-Salam and L. Carlitz (1965) Some orthogonal q -polynomials. Math. Nachr. 30, pp. 47–61.
  • N. W. Ashcroft and N. D. Mermin (1976) Solid State Physics. Holt, Rinehart and Winston, New York.
  • R. Askey (1975b) Orthogonal Polynomials and Special Functions. CBMS-NSF Regional Conference Series in Applied Mathematics, Vol. 21, Society for Industrial and Applied Mathematics, Philadelphia, PA.
  • R. Askey (1989) Continuous q -Hermite Polynomials when q > 1 . In q -series and Partitions (Minneapolis, MN, 1988), IMA Vol. Math. Appl., Vol. 18, pp. 151–158.
  • J. Avron and B. Simon (1982) Singular Continuous Spectrum for a Class of Almost Periodic Jacobi Matrices. Bulletin of the American Mathematical Society 6 (1), pp. 81–85.
  • 3: 24.2 Definitions and Generating Functions
    24.2.3 t e x t e t 1 = n = 0 B n ( x ) t n n ! , | t | < 2 π .
    24.2.8 2 e x t e t + 1 = n = 0 E n ( x ) t n n ! , | t | < π ,
    Table 24.2.3: Bernoulli numbers B n = N / D .
    n N D B n
    30 861 58412 76005 14322 6.01580 8739 ×10⁸
    Table 24.2.4: Euler numbers E n .
    n E n
    30 44 15438 93249 02310 45536 82821
    Table 24.2.5: Coefficients b n , k of the Bernoulli polynomials B n ( x ) = k = 0 n b n , k x k .
    k
    11 0 5 6 0 11 2 0 11 0 11 0 55 6 11 2 1
    4: Bibliography E
  • A. R. Edmonds (1974) Angular Momentum in Quantum Mechanics. 3rd printing, with corrections, 2nd edition, Princeton University Press, Princeton, NJ.
  • U. T. Ehrenmark (1995) The numerical inversion of two classes of Kontorovich-Lebedev transform by direct quadrature. J. Comput. Appl. Math. 61 (1), pp. 43–72.
  • Á. Elbert and A. Laforgia (1997) An upper bound for the zeros of the derivative of Bessel functions. Rend. Circ. Mat. Palermo (2) 46 (1), pp. 123–130.
  • G. A. Evans and J. R. Webster (1999) A comparison of some methods for the evaluation of highly oscillatory integrals. J. Comput. Appl. Math. 112 (1-2), pp. 55–69.
  • H. Exton (1983) The asymptotic behaviour of the inhomogeneous Airy function Hi ( z ) . Math. Chronicle 12, pp. 99–104.
  • 5: Bibliography L
  • Soo-Y. Lee (1980) The inhomogeneous Airy functions, Gi ( z )  and Hi ( z ) . J. Chem. Phys. 72 (1), pp. 332–336.
  • S. Lewanowicz (1991) Evaluation of Bessel function integrals with algebraic singularities. J. Comput. Appl. Math. 37 (1-3), pp. 101–112.
  • E. R. Love (1972b) Two index laws for fractional integrals and derivatives. J. Austral. Math. Soc. 14, pp. 385–410.
  • J. Lund (1985) Bessel transforms and rational extrapolation. Numer. Math. 47 (1), pp. 1–14.
  • J. N. Lyness (1985) Integrating some infinite oscillating tails. J. Comput. Appl. Math. 12/13, pp. 109–117.
  • 6: Bibliography C
  • R. G. Campos (1995) A quadrature formula for the Hankel transform. Numer. Algorithms 9 (2), pp. 343–354.
  • S. M. Candel (1981) An algorithm for the Fourier-Bessel transform. Comput. Phys. Comm. 23 (4), pp. 343–353.
  • B. C. Carlson (2011) Permutation symmetry for theta functions. J. Math. Anal. Appl. 378 (1), pp. 42–48.
  • N. B. Christensen (1990) Optimized fast Hankel transform filters. Geophysical Prospecting 38 (5), pp. 545–568.
  • P. Cornille (1972) Computation of Hankel transforms. SIAM Rev. 14 (2), pp. 278–285.
  • 7: 9.18 Tables
  • Miller (1946) tabulates Ai ( x ) , Ai ( x ) for x = 20 ( .01 ) 2 ; log 10 Ai ( x ) , Ai ( x ) / Ai ( x ) for x = 0 ( .1 ) 25 ( 1 ) 75 ; Bi ( x ) , Bi ( x ) for x = 10 ( .1 ) 2.5 ; log 10 Bi ( x ) , Bi ( x ) / Bi ( x ) for x = 0 ( .1 ) 10 ; M ( x ) , N ( x ) , θ ( x ) , ϕ ( x ) (respectively F ( x ) , G ( x ) , χ ( x ) , ψ ( x ) ) for x = 80 ( 1 ) 30 ( .1 ) 0 . Precision is generally 8D; slightly less for some of the auxiliary functions. Extracts from these tables are included in Abramowitz and Stegun (1964, Chapter 10), together with some auxiliary functions for large arguments.

  • 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.

  • 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.

  • §9.18(vii) Generalized Airy Functions
    8: Bibliography G
  • B. Gabutti (1979) On high precision methods for computing integrals involving Bessel functions. Math. Comp. 33 (147), pp. 1049–1057.
  • J. A. Gaunt (1929) The triplets of helium. Philos. Trans. Roy. Soc. London Ser. A 228, pp. 151–196.
  • A. Gil, J. Segura, and N. M. Temme (2002c) Computing complex Airy functions by numerical quadrature. Numer. Algorithms 30 (1), pp. 11–23.
  • G. H. Golub and C. F. Van Loan (1996) Matrix Computations. 3rd edition, Johns Hopkins University Press, Baltimore, MD.
  • R. G. Gordon (1970) Constructing wavefunctions for nonlocal potentials. J. Chem. Phys. 52, pp. 6211–6217.
  • 9: Bibliography B
  • W. N. Bailey (1938) The generating function of Jacobi polynomials. J. London Math. Soc. 13, pp. 8–12.
  • R. Barakat and E. Parshall (1996) Numerical evaluation of the zero-order Hankel transform using Filon quadrature philosophy. Appl. Math. Lett. 9 (5), pp. 21–26.
  • A. R. Barnett (1981b) KLEIN: Coulomb functions for real λ and positive energy to high accuracy. Comput. Phys. Comm. 24 (2), pp. 141–159.
  • V. Bezvoda, R. Farzan, K. Segeth, and G. Takó (1986) On numerical evaluation of integrals involving Bessel functions. Apl. Mat. 31 (5), pp. 396–410.
  • A. Burgess (1963) The determination of phases and amplitudes of wave functions. Proc. Phys. Soc. 81 (3), pp. 442–452.
  • 10: Bibliography O
  • K. Okamoto (1987a) Studies on the Painlevé equations. I. Sixth Painlevé equation P VI . Ann. Mat. Pura Appl. (4) 146, pp. 337–381.
  • F. W. J. Olver (1951) A further method for the evaluation of zeros of Bessel functions and some new asymptotic expansions for zeros of functions of large order. Proc. Cambridge Philos. Soc. 47, pp. 699–712.
  • F. W. J. Olver (1952) Some new asymptotic expansions for Bessel functions of large orders. Proc. Cambridge Philos. Soc. 48 (3), pp. 414–427.
  • F. W. J. Olver (1959) Uniform asymptotic expansions for Weber parabolic cylinder functions of large orders. J. Res. Nat. Bur. Standards Sect. B 63B, pp. 131–169.
  • J. M. Ortega and W. C. Rheinboldt (1970) Iterative Solution of Nonlinear Equations in Several Variables. Academic Press, New York.