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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: 19.2 Definitions
β–ΊThe integral for E ⁑ ( Ο• , k ) is well defined if k 2 = sin 2 ⁑ Ο• = 1 , and the Cauchy principal value (§1.4(v)) of Ξ  ⁑ ( Ο• , Ξ± 2 , k ) is taken if 1 Ξ± 2 ⁒ sin 2 ⁑ Ο• vanishes at an interior point of the integration path. … β–ΊThe principal branch of K ⁑ ( k ) and E ⁑ ( k ) is | ph ⁑ ( 1 k 2 ) | Ο€ , that is, the branch-cuts are ( , 1 ] [ 1 , + ) . The principal values of K ⁑ ( k ) and E ⁑ ( k ) are even functions. … β–Ί
§19.2(iv) A Related Function: R C ⁑ ( x , y )
β–ΊFor the special cases of R C ⁑ ( x , x ) and R C ⁑ ( 0 , y ) see (19.6.15). …
3: 34.12 Physical Applications
§34.12 Physical Applications
β–ΊThe angular momentum coupling coefficients ( 3 ⁒ j , 6 ⁒ j , and 9 ⁒ j symbols) are essential in the fields of nuclear, atomic, and molecular physics. … 3 ⁒ j , 6 ⁒ j , and 9 ⁒ j symbols are also found in multipole expansions of solutions of the Laplace and Helmholtz equations; see Carlson and Rushbrooke (1950) and Judd (1976).
4: 9 Airy and Related Functions
Chapter 9 Airy and Related Functions
5: Bibliography
β–Ί
  • M. Abramowitz and P. Rabinowitz (1954) Evaluation of Coulomb wave functions along the transition line. Physical Rev. (2) 96, pp. 77–79.
  • β–Ί
  • D. E. Amos (1983c) Uniform asymptotic expansions for exponential integrals E n ⁒ ( x ) and Bickley functions Ki n ⁒ ( x ) . ACM Trans. Math. Software 9 (4), pp. 467–479.
  • β–Ί
  • T. M. Apostol (1952) Theorems on generalized Dedekind sums. Pacific J. Math. 2 (1), pp. 1–9.
  • β–Ί
  • H. Appel (1968) Numerical Tables for Angular Correlation Computations in Ξ± -, Ξ² - and Ξ³ -Spectroscopy: 3 ⁒ j -, 6 ⁒ j -, 9 ⁒ j -Symbols, F- and Ξ“ -Coefficients. Landolt-Börnstein Numerical Data and Functional Relationships in Science and Technology, Springer-Verlag.
  • β–Ί
  • F. M. Arscott (1959) A new treatment of the ellipsoidal wave equation. Proc. London Math. Soc. (3) 9, pp. 21–50.
  • 6: 34 3j, 6j, 9j Symbols
    Chapter 34 3 ⁒ j , 6 ⁒ j , 9 ⁒ j Symbols
    7: 34.14 Tables
    §34.14 Tables
    β–ΊTables of exact values of the squares of the 3 ⁒ j and 6 ⁒ j symbols in which all parameters are 8 are given in Rotenberg et al. (1959), together with a bibliography of earlier tables of 3 ⁒ j , 6 ⁒ j , and 9 ⁒ j symbols on pp. … β–ΊSome selected 9 ⁒ j symbols are also given. … 16-17; for 9 ⁒ j symbols on p. … β–Ί 310–332, and for the 9 ⁒ j symbols on pp. …
    8: 26.6 Other Lattice Path Numbers
    β–Ί
    Delannoy Number D ⁑ ( m , n )
    β–Ί D ⁑ ( m , n ) is the number of paths from ( 0 , 0 ) to ( m , n ) that are composed of directed line segments of the form ( 1 , 0 ) , ( 0 , 1 ) , or ( 1 , 1 ) . … β–Ί
    Table 26.6.4: Schröder numbers r ⁑ ( n ) .
    β–Ί β–Ίβ–Ίβ–Ί
    n r ⁑ ( n ) n r ⁑ ( n ) n r ⁑ ( n ) n r ⁑ ( n ) n r ⁑ ( n )
    1 2 5 394 9 2 06098 13 1420 78746 17 11 18180 26018
    β–Ί
    β–Ί
    26.6.12 C ⁑ ( n ) = k = 1 n N ⁑ ( n , k ) ,
    β–Ί
    26.6.13 M ⁑ ( n ) = k = 0 n ( 1 ) k ⁒ ( n k ) ⁒ C ⁑ ( n + 1 k ) ,
    9: 19.37 Tables
    β–Ί
    Functions K ⁑ ( k ) and E ⁑ ( k )
    β–ΊTabulated for k 2 = 0 ⁒ ( .01 ) ⁒ 1 to 6D by Byrd and Friedman (1971), to 15D for K ⁑ ( k ) and 9D for E ⁑ ( k ) by Abramowitz and Stegun (1964, Chapter 17), and to 10D by Fettis and Caslin (1964). … β–Ί
    Functions F ⁑ ( Ο• , k ) and E ⁑ ( Ο• , k )
    β–ΊTabulated for Ο• = 0 ⁒ ( 5 ∘ ) ⁒ 90 ∘ , arcsin ⁑ k = 0 ⁒ ( 1 ∘ ) ⁒ 90 ∘ to 6D by Byrd and Friedman (1971), for Ο• = 0 ⁒ ( 5 ∘ ) ⁒ 90 ∘ , arcsin ⁑ k = 0 ⁒ ( 2 ∘ ) ⁒ 90 ∘ and 5 ∘ ⁒ ( 10 ∘ ) ⁒ 85 ∘ to 8D by Abramowitz and Stegun (1964, Chapter 17), and for Ο• = 0 ⁒ ( 10 ∘ ) ⁒ 90 ∘ , arcsin ⁑ k = 0 ⁒ ( 5 ∘ ) ⁒ 90 ∘ to 9D by Zhang and Jin (1996, pp. 674–675). … β–ΊTabulated for Ο• = 5 ∘ ⁒ ( 5 ∘ ) ⁒ 80 ∘ ⁒ ( 2.5 ∘ ) ⁒ 90 ∘ , Ξ± 2 = 1 ⁒ ( .1 ) 0.1 , 0.1 ⁒ ( .1 ) ⁒ 1 , k 2 = 0 ⁒ ( .05 ) ⁒ 0.9 ⁒ ( .02 ) ⁒ 1 to 10D by Fettis and Caslin (1964) (and warns of inaccuracies in Selfridge and Maxfield (1958) and Paxton and Rollin (1959)). …
    10: Bibliography L
    β–Ί
  • 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.
  • β–Ί
  • J. L. López, P. Pagola, and E. Pérez Sinusía (2013b) Asymptotics of the first Appell function F 1 with large parameters. Integral Transforms Spec. Funct. 24 (9), pp. 715–733.
  • β–Ί
  • 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.