About the Project

/shop/%E2%99%9F%F0%9F%AA%90%F0%9F%A6%B8%20Buy%20DNP%20Online%20$0.99%20Per%20Capsule%3A%20%F0%9F%92%A3%20www.BuyDNPOnline.cc%20%F0%9F%92%A3%20Buy%20DNP%20UK%20%F0%9F%A6%B8%F0%9F%AA%90%E2%99%9F%20Buy%20DNP%20In%20Australia%20-%20Buy%20DNP-www.BuyDNPOnline.cc

AdvancedHelp

(0.042 seconds)

21—30 of 983 matching pages

21: 16.4 Argument Unity
The function F q q + 1 ( 𝐚 ; 𝐛 ; z ) is well-poised if … See Raynal (1979) for a statement in terms of 3 j symbols (Chapter 34). … Transformations for both balanced F 3 4 ( 1 ) and very well-poised F 6 7 ( 1 ) are included in Bailey (1964, pp. 56–63). A similar theory is available for very well-poised F 8 9 ( 1 ) ’s which are 2-balanced. …
22: 15.8 Transformations of Variable
All functions in this subsection and §15.8(ii) assume their principal values. … When b a is an integer limits are taken in (15.8.2) and (15.8.3) as follows. … In (15.8.8) when c a k m is a nonpositive integer ψ ( c a k m ) / Γ ( c a k m ) is interpreted as ( 1 ) m + k + a c + 1 ( m + k + a c ) ! . … Alternatively, if b a is a negative integer, then we interchange a and b in 𝐅 ( a , b ; c ; z ) . In a similar way, when c a b is an integer limits are taken in (15.8.4) and (15.8.5) as follows. …
23: Bibliography M
  • P. Martín, R. Pérez, and A. L. Guerrero (1992) Two-point quasi-fractional approximations to the Airy function Ai ( x ) . J. Comput. Phys. 99 (2), pp. 337–340.
  • J. McMahon (1894) On the roots of the Bessel and certain related functions. Ann. of Math. 9 (1-6), pp. 23–30.
  • J. Meixner (1934) Orthogonale Polynomsysteme mit einer besonderen Gestalt der erzeugenden Funktion. J. Lond. Math. Soc. 9, pp. 6–13 (German).
  • P. Midy (1975) An improved calculation of the general elliptic integral of the second kind in the neighbourhood of x = 0 . Numer. Math. 25 (1), pp. 99–101.
  • T. Morita (2013) A connection formula for the q -confluent hypergeometric function. SIGMA Symmetry Integrability Geom. Methods Appl. 9, pp. Paper 050, 13.
  • 24: Bibliography S
  • H. E. Salzer (1955) Orthogonal polynomials arising in the numerical evaluation of inverse Laplace transforms. Math. Tables Aids Comput. 9 (52), pp. 164–177.
  • J. Segura and A. Gil (1999) Evaluation of associated Legendre functions off the cut and parabolic cylinder functions. Electron. Trans. Numer. Anal. 9, pp. 137–146.
  • D. C. Shaw (1985) Perturbational results for diffraction of water-waves by nearly-vertical barriers. IMA J. Appl. Math. 34 (1), pp. 99–117.
  • K. Srinivasa Rao, V. Rajeswari, and C. B. Chiu (1989) A new Fortran program for the 9 - j angular momentum coefficient. Comput. Phys. Comm. 56 (2), pp. 231–248.
  • S. K. Suslov (2003) An Introduction to Basic Fourier Series. Developments in Mathematics, Vol. 9, Kluwer Academic Publishers, Dordrecht.
  • 25: 19.5 Maclaurin and Related Expansions
    where F 1 2 is the Gauss hypergeometric function (§§15.1 and 15.2(i)). …where F 1 ( α ; β , β ; γ ; x , y ) is an Appell function (§16.13). … Coefficients of terms up to λ 49 are given in Lee (1990), along with tables of fractional errors in K ( k ) and E ( k ) , 0.1 k 2 0.9999 , obtained by using 12 different truncations of (19.5.6) in (19.5.8) and (19.5.9). … Series expansions of F ( ϕ , k ) and E ( ϕ , k ) are surveyed and improved in Van de Vel (1969), and the case of F ( ϕ , k ) is summarized in Gautschi (1975, §1.3.2). For series expansions of Π ( ϕ , α 2 , k ) when | α 2 | < 1 see Erdélyi et al. (1953b, §13.6(9)). …
    26: 19.21 Connection Formulas
    The complete cases of R F and R G have connection formulas resulting from those for the Gauss hypergeometric function (Erdélyi et al. (1953a, §2.9)). … The complete case of R J can be expressed in terms of R F and R D : … R D ( x , y , z ) is symmetric only in x and y , but either (nonzero) x or (nonzero) y can be moved to the third position by using …Because R G is completely symmetric, x , y , z can be permuted on the right-hand side of (19.21.10) so that ( x z ) ( y z ) 0 if the variables are real, thereby avoiding cancellations when R G is calculated from R F and R D (see §19.36(i)). … Connection formulas for R a ( 𝐛 ; 𝐳 ) are given in Carlson (1977b, pp. 99, 101, and 123–124). …
    27: 34.4 Definition: 6 j Symbol
    §34.4 Definition: 6 j Symbol
    The 6 j symbol is defined by the following double sum of products of 3 j symbols: …where the summation is taken over all admissible values of the m ’s and m ’s for each of the four 3 j symbols; compare (34.2.2) and (34.2.3). … where F 3 4 is defined as in §16.2. For alternative expressions for the 6 j symbol, written either as a finite sum or as other terminating generalized hypergeometric series F 3 4 of unit argument, see Varshalovich et al. (1988, §§9.2.1, 9.2.3).
    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: 18.13 Continued Fractions
    The following formulae are explicit cases of (18.2.34)–(18.2.36); this area is fully explored in §§18.30(vi) and 18.30(vii). …
    18.13.3 a 1 x + 1 2 3 2 x + 2 3 5 3 x + 3 4 7 4 x + ,
    18.13.4 a 1 1 x + 1 2 1 2 ( 3 x ) + 2 3 1 3 ( 5 x ) + 3 4 1 4 ( 7 x ) + ,
    See also Cuyt et al. (2008, pp. 91–99).
    30: 34.10 Zeros
    §34.10 Zeros
    In a 3 j symbol, if the three angular momenta j 1 , j 2 , j 3 do not satisfy the triangle conditions (34.2.1), or if the projective quantum numbers do not satisfy (34.2.3), then the 3 j symbol is zero. Similarly the 6 j symbol (34.4.1) vanishes when the triangle conditions are not satisfied by any of the four 3 j symbols in the summation. …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).