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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: Bibliography H
β–Ί
  • M. H. Halley, D. Delande, and K. T. Taylor (1993) The combination of R -matrix and complex coordinate methods: Application to the diamagnetic Rydberg spectra of Ba and Sr. J. Phys. B 26 (12), pp. 1775–1790.
  • β–Ί
  • B. A. Hargrave and B. D. Sleeman (1977) Lamé polynomials of large order. SIAM J. Math. Anal. 8 (5), pp. 800–842.
  • β–Ί
  • J. R. Herndon (1961b) Algorithm 56: Complete elliptic integral of the second kind. Comm. ACM 4 (4), pp. 180–181.
  • β–Ί
  • L. E. Hoisington and G. Breit (1938) Calculation of Coulomb wave functions for high energies. Phys. Rev. 54 (8), pp. 627–628.
  • β–Ί
  • M. H. Hull and G. Breit (1959) Coulomb Wave Functions. In Handbuch der Physik, Bd. 41/1, S. Flügge (Ed.), pp. 408–465.
  • 3: 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 26.6.1: Delannoy numbers D ⁑ ( m , n ) .
    β–Ί β–Ίβ–Ίβ–Ί
    m n
    0 1 2 3 4 5 6 7 8 9 10
    β–Ί
    β–Ί
    Table 26.6.2: Motzkin numbers M ⁑ ( n ) .
    β–Ί β–Ίβ–Ίβ–Ί
    n M ⁑ ( n ) n M ⁑ ( n ) n M ⁑ ( n ) n M ⁑ ( n ) n M ⁑ ( n )
    0 1 4 9 8 323 12 15511 16 8 53467
    β–Ί
    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 )
    0 1 4 90 8 41586 12 272 97738 16 2 09271 56706
    β–Ί
    4: 19.37 Tables
    β–Ί
    Functions F ⁑ ( Ο• , k ) and E ⁑ ( Ο• , k )
    β–Ί( F ⁑ ( Ο• , k ) is presented as Ξ  ⁑ ( Ο• , 0 , 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)). … β–Ί
    Function R F ⁑ ( a 2 , b 2 , c 2 ) with a ⁒ b ⁒ c = 1
    5: 27.2 Functions
    β–Ί( Ξ½ ⁑ ( 1 ) is defined to be 0.) …It can be expressed as a sum over all primes p x : … 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 . …
    6: 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 (1983b) Algorithm 610. A portable FORTRAN subroutine for derivatives of the psi function. ACM Trans. Math. Software 9 (4), pp. 494–502.
  • 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.
  • 7: 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).
    8: 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. …
    9: 1.12 Continued Fractions
    β–Ί C n is called the n th approximant or convergent to C . A n and B n are called the n th (canonical) numerator and denominator respectively. … β–ΊDefine … β–ΊConversely, C is called an extension of C . … β–ΊThen the convergents C n satisfy …
    10: 9 Airy and Related Functions
    Chapter 9 Airy and Related Functions