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1: 34.2 Definition: 3 j Symbol
§34.2 Definition: 3 j Symbol
The quantities j 1 , j 2 , j 3 in the 3 j symbol are called angular momenta. …They therefore satisfy the triangle conditions …where r , s , t is any permutation of 1 , 2 , 3 . The corresponding projective quantum numbers m 1 , m 2 , m 3 are given by …
2: Bibliography
  • J. C. Adams and P. N. Swarztrauber (1997) SPHEREPACK 2.0: A Model Development Facility. NCAR Technical Note Technical Report TN-436-STR, National Center for Atmospheric Research.
  • H. Alzer (2000) Sharp bounds for the Bernoulli numbers. Arch. Math. (Basel) 74 (3), pp. 207–211.
  • D. E. Amos (1980b) Computation of exponential integrals. ACM Trans. Math. Software 6 (3), pp. 365–377.
  • G. E. Andrews (1966b) q -identities of Auluck, Carlitz, and Rogers. Duke Math. J. 33 (3), pp. 575–581.
  • G. E. Andrews (1979) Plane partitions. III. The weak Macdonald conjecture. Invent. Math. 53 (3), pp. 193–225.
  • 3: Software Index
    Open Source With Book Commercial
    34 3j, 6j, 9j Symbols
  • Open Source Collections and Systems.

    These are collections of software (e.g. libraries) or interactive systems of a somewhat broad scope. Contents may be adapted from research software or may be contributed by project participants who donate their services to the project. The software is made freely available to the public, typically in source code form. While formal support of the collection may not be provided by its developers, within active projects there is often a core group who donate time to consider bug reports and make updates to the collection.

  • 4: 34.11 Higher-Order 3 n j Symbols
    §34.11 Higher-Order 3 n j Symbols
    5: 4.17 Special Values and Limits
    Table 4.17.1: Trigonometric functions: values at multiples of 1 12 π .
    θ sin θ cos θ tan θ csc θ sec θ cot θ
    π / 12 1 4 2 ( 3 1 ) 1 4 2 ( 3 + 1 ) 2 3 2 ( 3 + 1 ) 2 ( 3 1 ) 2 + 3
    π / 6 1 2 1 2 3 1 3 3 2 2 3 3 3
    π / 3 1 2 3 1 2 3 2 3 3 2 1 3 3
    2 π / 3 1 2 3 1 2 3 2 3 3 2 1 3 3
    5 π / 6 1 2 1 2 3 1 3 3 2 2 3 3 3
    6: 34.12 Physical Applications
    §34.12 Physical Applications
    The 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).
    7: 34.3 Basic Properties: 3 j Symbol
    §34.3 Basic Properties: 3 j Symbol
    §34.3(ii) Symmetry
    §34.3(iv) Orthogonality
    §34.3(vi) Sums
    8: 34.5 Basic Properties: 6 j Symbol
    34.5.6 { j 1 j 2 j 3 1 j 3 1 j 2 + 1 } = ( 1 ) J ( ( J 2 j 2 1 ) ( J 2 j 2 ) ( J 2 j 3 + 1 ) ( J 2 j 3 + 2 ) ( 2 j 2 + 1 ) ( 2 j 2 + 2 ) ( 2 j 2 + 3 ) ( 2 j 3 1 ) 2 j 3 ( 2 j 3 + 1 ) ) 1 2 ,
    34.5.9 { j 1 j 2 j 3 l 1 l 2 l 3 } = { j 1 1 2 ( j 2 + l 2 + j 3 l 3 ) 1 2 ( j 2 l 2 + j 3 + l 3 ) l 1 1 2 ( j 2 + l 2 j 3 + l 3 ) 1 2 ( j 2 + l 2 + j 3 + l 3 ) } ,
    34.5.14 j 3 ( 2 j 3 + 1 ) ( 2 l 3 + 1 ) { j 1 j 2 j 3 l 1 l 2 l 3 } { j 1 j 2 j 3 l 1 l 2 l 3 } = δ l 3 , l 3 .
    34.5.16 ( 1 ) j 1 + j 2 + j 3 + j 1 + j 2 + l 1 + l 2 { j 1 j 2 j 3 l 1 l 2 l 3 } { j 1 j 2 j 3 l 1 l 2 l 3 } = j ( 1 ) l 3 + l 3 + j ( 2 j + 1 ) { j 1 j 1 j j 2 j 2 j 3 } { l 3 l 3 j j 1 j 1 l 2 } { l 3 l 3 j j 2 j 2 l 1 } .
    34.5.23 ( j 1 j 2 j 3 m 1 m 2 m 3 ) { j 1 j 2 j 3 l 1 l 2 l 3 } = m 1 m 2 m 3 ( 1 ) l 1 + l 2 + l 3 + m 1 + m 2 + m 3 ( j 1 l 2 l 3 m 1 m 2 m 3 ) ( l 1 j 2 l 3 m 1 m 2 m 3 ) ( l 1 l 2 j 3 m 1 m 2 m 3 ) .
    9: 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). Except in degenerate cases the combination of the triangle inequalities for the four 3 j symbols in (34.4.1) is equivalent to the existence of a tetrahedron (possibly degenerate) with edges of lengths j 1 , j 2 , j 3 , l 1 , l 2 , l 3 ; see Figure 34.4.1. … where F 3 4 is defined as in §16.2. …
    10: 34.1 Special Notation
    The main functions treated in this chapter are the Wigner 3 j , 6 j , 9 j symbols, respectively,
    ( j 1 j 2 j 3 m 1 m 2 m 3 ) ,
    { j 1 j 2 j 3 l 1 l 2 l 3 } ,
    An often used alternative to the 3 j symbol is the Clebsch–Gordan coefficient …For other notations for 3 j , 6 j , 9 j symbols, see Edmonds (1974, pp. 52, 97, 104–105) and Varshalovich et al. (1988, §§8.11, 9.10, 10.10).