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Watson 3F2 sum

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1: 34.2 Definition: 3 j Symbol
§34.2 Definition: 3 j Symbol
The corresponding projective quantum numbers m 1 , m 2 , m 3 are given by … When both conditions are satisfied the 3 j symbol can be expressed as the finite sumwhere F 2 3 is defined as in §16.2. For alternative expressions for the 3 j symbol, written either as a finite sum or as other terminating generalized hypergeometric series F 2 3 of unit argument, see Varshalovich et al. (1988, §§8.21, 8.24–8.26).
2: 20.8 Watson’s Expansions
§20.8 Watson’s Expansions
20.8.1 θ 2 ( 0 , q ) θ 3 ( z , q ) θ 4 ( z , q ) θ 2 ( z , q ) = 2 n = ( 1 ) n q n 2 e i 2 n z q n e i z + q n e i z .
See Watson (1935a). …
3: 16.24 Physical Applications
§16.24(i) Random Walks
Generalized hypergeometric functions and Appell functions appear in the evaluation of the so-called Watson integrals which characterize the simplest possible lattice walks. …
§16.24(iii) 3 j , 6 j , and 9 j Symbols
The 3 j symbols, or Clebsch–Gordan coefficients, play an important role in the decomposition of reducible representations of the rotation group into irreducible representations. They can be expressed as F 2 3 functions with unit argument. …
4: 11 Struve and Related Functions
5: 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. …
34.8.1 { j 1 j 2 j 3 j 2 j 1 l 3 } = ( 1 ) j 1 + j 2 + j 3 + l 3 ( 4 π ( 2 j 1 + 1 ) ( 2 j 2 + 1 ) ( 2 l 3 + 1 ) sin θ ) 1 2 ( cos ( ( l 3 + 1 2 ) θ 1 4 π ) + o ( 1 ) ) , j 1 , j 2 , j 3 l 3 1 ,
Uniform approximations in terms of Airy functions for the 3 j and 6 j symbols are given in Schulten and Gordon (1975b). 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.
6: 10 Bessel Functions
7: 10.42 Zeros
The distribution of the zeros of K n ( n z ) in the sector 3 2 π ph z 1 2 π in the cases n = 1 , 5 , 10 is obtained on rotating Figures 10.21.2, 10.21.4, 10.21.6, respectively, through an angle 1 2 π so that in each case the cut lies along the positive imaginary axis. The zeros in the sector 1 2 π ph z 3 2 π are their conjugates. … For the number of zeros of K ν ( z ) in the sector | ph z | π , when ν is real, see Watson (1944, pp. 511–513). …
8: 27.21 Tables
Glaisher (1940) contains four tables: Table I tabulates, for all n 10 4 : (a) the canonical factorization of n into powers of primes; (b) the Euler totient ϕ ( n ) ; (c) the divisor function d ( n ) ; (d) the sum σ ( n ) of these divisors. … The partition function p ( n ) is tabulated in Gupta (1935, 1937), Watson (1937), and Gupta et al. (1958). Tables of the Ramanujan function τ ( n ) are published in Lehmer (1943) and Watson (1949). …
9: Bibliography W
  • G. N. Watson (1910) The cubic transformation of the hypergeometric function. Quart. J. Pure and Applied Math. 41, pp. 70–79.
  • G. N. Watson (1935a) Generating functions of class-numbers. Compositio Math. 1, pp. 39–68.
  • G. N. Watson (1935b) The surface of an ellipsoid. Quart. J. Math., Oxford Ser. 6, pp. 280–287.
  • G. N. Watson (1937) Two tables of partitions. Proc. London Math. Soc. (2) 42, pp. 550–556.
  • G. N. Watson (1949) A table of Ramanujan’s function τ ( n ) . Proc. London Math. Soc. (2) 51, pp. 1–13.
  • 10: 20.7 Identities
    §20.7(i) Sums of Squares
    For these and similar formulas see Lawden (1989, §1.4), Whittaker and Watson (1927, pp. 487–488), and Carlson (2011, §5). Also, in further development along the lines of the notations of Neville (§20.1) and of Glaisher (§22.2), the identities (20.7.6)–(20.7.9) have been recast in a more symmetric manner with respect to suffices 2 , 3 , 4 . …
    §20.7(v) Watson’s Identities
    See also Carlson (2011, §3). …