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11—17 of 17 matching pages

11: 16.24 Physical Applications
§16.24(iii) 3 j , 6 j , and 9 j Symbols
The coefficients of transformations between different coupling schemes of three angular momenta are related to the Wigner 6 j symbols. …
12: 34.7 Basic Properties: 9 j Symbol
34.7.1 { j 11 j 12 j 13 j 21 j 22 j 13 j 31 j 31 0 } = ( 1 ) j 12 + j 21 + j 13 + j 31 ( ( 2 j 13 + 1 ) ( 2 j 31 + 1 ) ) 1 2 { j 11 j 12 j 13 j 22 j 21 j 31 } .
34.7.5 j ( 2 j + 1 ) { j 11 j 12 j j 21 j 22 j 23 j 31 j 32 j 33 } { j 11 j 12 j j 23 j 33 j } = ( 1 ) 2 j { j 21 j 22 j 23 j 12 j j 32 } { j 31 j 32 j 33 j j 11 j 21 } .
13: 16.7 Relations to Other Functions
For 3 j , 6 j , 9 j symbols see Chapter 34. …
14: 34.3 Basic Properties: 3 j Symbol
Similar conventions apply to all subsequent summations in this chapter.
15: 34 3j, 6j, 9j Symbols
Chapter 34 3 j , 6 j , 9 j Symbols
16: 16.4 Argument Unity
See Raynal (1979) for a statement in terms of 3 j symbols (Chapter 34). … These series contain 6 j symbols as special cases when the parameters are integers; compare §34.4. …
17: Errata
  • Section 34.1

    The relation between Clebsch-Gordan and 3 j symbols was clarified, and the sign of m 3 was changed for readability. The reference Condon and Shortley (1935) for the Clebsch-Gordan coefficients was replaced by Edmonds (1974) and Rotenberg et al. (1959) and the references for 3 j , 6 j , 9 j symbols were made more precise in §34.1.

  • Section 34.1

    The reference for Clebsch-Gordan coefficients, Condon and Shortley (1935), was replaced by Edmonds (1974) and Rotenberg et al. (1959). The references for 3 j , 6 j , 9 j symbols were made more precise.