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1: 34.6 Definition: 9 ⁒ j Symbol
§34.6 Definition: 9 ⁒ j Symbol
β–ΊThe 9 ⁒ j symbol may be defined either in terms of 3 ⁒ j symbols or equivalently in terms of 6 ⁒ j symbols: β–Ί
34.6.1 { j 11 j 12 j 13 j 21 j 22 j 23 j 31 j 32 j 33 } = all  ⁒ m r ⁒ s ( j 11 j 12 j 13 m 11 m 12 m 13 ) ⁒ ( j 21 j 22 j 23 m 21 m 22 m 23 ) ⁒ ( j 31 j 32 j 33 m 31 m 32 m 33 ) ⁒ ( j 11 j 21 j 31 m 11 m 21 m 31 ) ⁒ ( j 12 j 22 j 32 m 12 m 22 m 32 ) ⁒ ( j 13 j 23 j 33 m 13 m 23 m 33 ) ,
β–Ί
34.6.2 { j 11 j 12 j 13 j 21 j 22 j 23 j 31 j 32 j 33 } = j ( 1 ) 2 ⁒ j ⁒ ( 2 ⁒ j + 1 ) ⁒ { j 11 j 21 j 31 j 32 j 33 j } ⁒ { j 12 j 22 j 32 j 21 j j 23 } ⁒ { j 13 j 23 j 33 j j 11 j 12 } .
β–ΊThe 9 ⁒ j symbol may also be written as a finite triple sum equivalent to a terminating generalized hypergeometric series of three variables with unit arguments. …
2: 9.13 Generalized Airy Functions
β–ΊSwanson and Headley (1967) define independent solutions A n ⁑ ( z ) and B n ⁑ ( z ) of (9.13.1) by … β–ΊProperties of A n ⁑ ( z ) and B n ⁑ ( z ) follow from the corresponding properties of the modified Bessel functions. … β–ΊThe distribution in β„‚ and asymptotic properties of the zeros of A n ⁑ ( z ) , A n ⁑ ( z ) , B n ⁑ ( z ) , and B n ⁑ ( z ) are investigated in Swanson and Headley (1967) and Headley and Barwell (1975). … β–ΊTheir relations to the functions A n ⁑ ( z ) and B n ⁑ ( z ) are given by … β–ΊThe A k ⁑ ( z , p ) are related by …
3: Bibliography L
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  • S. Lai and Y. Chiu (1992) Exact computation of the 9 - j symbols. Comput. Phys. Comm. 70 (3), pp. 544–556.
  • β–Ί
  • E. M. Lifshitz and L. P. PitaevskiΔ­ (1980) Statistical Physics, Part 2: Theory of the Condensed State. Pergamon Press, Oxford.
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  • Lord Kelvin (1905) Deep water ship-waves. Phil. Mag. 9, pp. 733–757.
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  • D. W. Lozier and F. W. J. Olver (1994) Numerical Evaluation of Special Functions. In Mathematics of Computation 1943–1993: A Half-Century of Computational Mathematics (Vancouver, BC, 1993), Proc. Sympos. Appl. Math., Vol. 48, pp. 79–125.
  • β–Ί
  • Y. L. Luke (1971a) Miniaturized tables of Bessel functions. II. Math. Comp. 25 (116), pp. 789–795 and D14–E13.
  • 4: 27.20 Methods of Computation: Other Number-Theoretic Functions
    β–ΊSee Calkin et al. (2007), and Lehmer (1941, pp. 5–83). …
    5: Bibliography D
    β–Ί
  • S. D. Daymond (1955) The principal frequencies of vibrating systems with elliptic boundaries. Quart. J. Mech. Appl. Math. 8 (3), pp. 361–372.
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  • K. Dilcher (1987b) Irreducibility of certain generalized Bernoulli polynomials belonging to quadratic residue class characters. J. Number Theory 25 (1), pp. 72–80.
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  • P. G. L. Dirichlet (1849) Über die Bestimmung der mittleren Werthe in der Zahlentheorie. Abhandlungen der Königlich Preussischen Akademie der Wissenschaften von 1849, pp. 69–83 (German).
  • β–Ί
  • G. Doetsch (1955) Handbuch der Laplace-Transformation. Bd. II. Anwendungen der Laplace-Transformation. 1. Abteilung. Birkhäuser Verlag, Basel und Stuttgart (German).
  • β–Ί
  • 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.
  • 6: 28.6 Expansions for Small q
    β–Ί
    28.6.2 a 1 ⁑ ( q ) = 1 + q 1 8 ⁒ q 2 1 64 ⁒ q 3 1 1536 ⁒ q 4 + 11 36864 ⁒ q 5 + 49 5 89824 ⁒ q 6 + 55 94 37184 ⁒ q 7 83 353 89440 ⁒ q 8 + β‹― ,
    β–Ί
    28.6.3 b 1 ⁑ ( q ) = 1 q 1 8 ⁒ q 2 + 1 64 ⁒ q 3 1 1536 ⁒ q 4 11 36864 ⁒ q 5 + 49 5 89824 ⁒ q 6 55 94 37184 ⁒ q 7 83 353 89440 ⁒ q 8 + β‹― ,
    β–ΊLeading terms of the of the power series for m = 7 , 8 , 9 , are: β–Ί
    28.6.14 a m ⁑ ( q ) b m ⁑ ( q ) } = m 2 + 1 2 ⁒ ( m 2 1 ) ⁒ q 2 + 5 ⁒ m 2 + 7 32 ⁒ ( m 2 1 ) 3 ⁒ ( m 2 4 ) ⁒ q 4 + 9 ⁒ m 4 + 58 ⁒ m 2 + 29 64 ⁒ ( m 2 1 ) 5 ⁒ ( m 2 4 ) ⁒ ( m 2 9 ) ⁒ q 6 + β‹― .
    β–ΊNumerical values of the radii of convergence ρ n ( j ) of the power series (28.6.1)–(28.6.14) for n = 0 , 1 , , 9 are given in Table 28.6.1. …
    7: Bibliography I
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  • E. L. Ince (1940b) Further investigations into the periodic Lamé functions. Proc. Roy. Soc. Edinburgh 60, pp. 83–99.
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  • A. Iserles, S. P. Nørsett, and S. Olver (2006) Highly Oscillatory Quadrature: The Story So Far. In Numerical Mathematics and Advanced Applications, A. Bermudez de Castro and others (Eds.), pp. 97–118.
  • 8: 27.2 Functions
    β–Ί
    27.2.9 d ⁑ ( n ) = d | n 1
    β–ΊIt is the special case k = 2 of the function d k ⁑ ( n ) that counts the number of ways of expressing n as the product of k factors, with the order of factors taken into account. …Note that Οƒ 0 ⁑ ( n ) = d ⁑ ( n ) . … β–ΊTable 27.2.2 tabulates the Euler totient function Ο• ⁑ ( n ) , the divisor function d ⁑ ( n ) ( = Οƒ 0 ⁑ ( n ) ), and the sum of the divisors Οƒ ⁑ ( n ) ( = Οƒ 1 ⁑ ( n ) ), for n = 1 ⁒ ( 1 ) ⁒ 52 . β–Ί
    Table 27.2.1: Primes.
    β–Ί β–Ίβ–Ίβ–Ί
    n p n p n + 10 p n + 20 p n + 30 p n + 40 p n + 50 p n + 60 p n + 70 p n + 80 p n + 90
    3 5 41 83 137 191 241 307 367 431 487
    β–Ί
    9: Bibliography E
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  • Á. Elbert (2001) Some recent results on the zeros of Bessel functions and orthogonal polynomials. J. Comput. Appl. Math. 133 (1-2), pp. 65–83.
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  • A. Erdélyi (1942b) The Fuchsian equation of second order with four singularities. Duke Math. J. 9 (1), pp. 48–58.
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  • D. Erricolo and G. Carluccio (2013) Algorithm 934: Fortran 90 subroutines to compute Mathieu functions for complex values of the parameter. ACM Trans. Math. Softw. 40 (1), pp. 8:1–8:19.
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  • T. Estermann (1959) On the representations of a number as a sum of three squares. Proc. London Math. Soc. (3) 9, pp. 575–594.
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  • J. A. Ewell (1990) A new series representation for ΞΆ ⁒ ( 3 ) . Amer. Math. Monthly 97 (3), pp. 219–220.
  • 10: 3.9 Acceleration of Convergence
    β–Ί
    Table 3.9.1: Shanks’ transformation for s n = j = 1 n ( 1 ) j + 1 ⁒ j 2 .
    β–Ί β–Ίβ–Ίβ–Ίβ–Ίβ–Ίβ–Ί
    n t n , 2 t n , 4 t n , 6 t n , 8 t n , 10
    3 0.82300 13550 14 0.82247 78118 35 0.82246 72851 83 0.82246 70397 56 0.82246 70335 90
    4 0.82221 76684 88 0.82246 28314 41 0.82246 69467 93 0.82246 70314 36 0.82246 70333 75
    8 0.82243 73137 33 0.82246 67719 32 0.82246 70301 49 0.82246 70333 73 0.82246 70334 23
    9 0.82248 70624 89 0.82246 71865 91 0.82246 70351 34 0.82246 70334 48 0.82246 70334 24
    β–Ί