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3j,6j,9j symbols

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11: 34.10 Zeros
§34.10 Zeros
Similarly the 6 j symbol (34.4.1) vanishes when the triangle conditions are not satisfied by any of the four 3 j symbols in the summation. …However, the 3 j and 6 j symbols may vanish for certain combinations of the angular momenta and projective quantum numbers even when the triangle conditions are fulfilled. Such zeros are called nontrivial zeros. For further information, including examples of nontrivial zeros and extensions to 9 j symbols, see Srinivasa Rao and Rajeswari (1993, pp. 133–215, 294–295, 299–310).
12: 34.13 Methods of Computation
Methods of computation for 3 j and 6 j symbols include recursion relations, see Schulten and Gordon (1975a), Luscombe and Luban (1998), and Edmonds (1974, pp. 42–45, 48–51, 97–99); summation of single-sum expressions for these symbols, see Varshalovich et al. (1988, §§8.2.6, 9.2.1) and Fang and Shriner (1992); evaluation of the generalized hypergeometric functions of unit argument that represent these symbols, see Srinivasa Rao and Venkatesh (1978) and Srinivasa Rao (1981). …
13: 16.7 Relations to Other Functions
For 3 j , 6 j , 9 j symbols see Chapter 34. …
14: 16.4 Argument Unity
See Raynal (1979) for a statement in terms of 3 j symbols (Chapter 34). …
15: 34.8 Approximations for Large Parameters
§34.8 Approximations for Large Parameters
For large values of the parameters in the 3 j , 6 j , and 9 j symbols, different asymptotic forms are obtained depending on which parameters are large. … For approximations for the 3 j , 6 j , and 9 j symbols with error bounds see Flude (1998), Chen et al. (1999), and Watson (1999): these references also cite earlier work.
16: 10.59 Integrals
10.59.1 e i b t 𝗃 n ( t ) d t = { π i n P n ( b ) , 1 < b < 1 , 1 2 π ( ± i ) n , b = ± 1 , 0 , ± b > 1 ,
17: 10.54 Integral Representations
10.54.1 𝗃 n ( z ) = z n 2 n + 1 n ! 0 π cos ( z cos θ ) ( sin θ ) 2 n + 1 d θ .
18: 34.6 Definition: 9 j Symbol
The 9 j symbol may be defined either in terms of 3 j symbols or equivalently in terms of 6 j symbols:
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 ) ,
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 } .
19: Software Index
20: 10.60 Sums
10.60.2 sin w w = n = 0 ( 2 n + 1 ) 𝗃 n ( v ) 𝗃 n ( u ) P n ( cos α ) .
10.60.11 n = 0 𝗃 n 2 ( z ) = Si ( 2 z ) 2 z .
10.60.12 n = 0 ( 2 n + 1 ) 𝗃 n 2 ( z ) = 1 ,
10.60.13 n = 0 ( 1 ) n ( 2 n + 1 ) 𝗃 n 2 ( z ) = sin ( 2 z ) 2 z ,
10.60.14 n = 0 ( 2 n + 1 ) ( 𝗃 n ( z ) ) 2 = 1 3 .