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1: 34.4 Definition: 6 j Symbol
34.4.1 { j 1 j 2 j 3 l 1 l 2 l 3 } = m r m s ( 1 ) l 1 + m 1 + l 2 + m 2 + l 3 + m 3 ( j 1 j 2 j 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 ) ,
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. …
34.4.2 { j 1 j 2 j 3 l 1 l 2 l 3 } = Δ ( j 1 j 2 j 3 ) Δ ( j 1 l 2 l 3 ) Δ ( l 1 j 2 l 3 ) Δ ( l 1 l 2 j 3 ) s ( 1 ) s ( s + 1 ) ! ( s j 1 j 2 j 3 ) ! ( s j 1 l 2 l 3 ) ! ( s l 1 j 2 l 3 ) ! ( s l 1 l 2 j 3 ) ! 1 ( j 1 + j 2 + l 1 + l 2 s ) ! ( j 2 + j 3 + l 2 + l 3 s ) ! ( j 3 + j 1 + l 3 + l 1 s ) ! ,
34.4.3 { j 1 j 2 j 3 l 1 l 2 l 3 } = ( 1 ) j 1 + j 3 + l 1 + l 3 Δ ( j 1 j 2 j 3 ) Δ ( j 2 l 1 l 3 ) ( j 1 j 2 + l 1 + l 2 ) ! ( j 2 + j 3 + l 2 + l 3 ) ! ( j 1 + j 3 + l 1 + l 3 + 1 ) ! Δ ( j 1 l 2 l 3 ) Δ ( j 3 l 1 l 2 ) ( j 1 j 2 + j 3 ) ! ( j 2 + l 1 + l 3 ) ! ( j 1 + l 2 + l 3 + 1 ) ! ( j 3 + l 1 + l 2 + 1 ) ! F 3 4 ( j 1 + j 2 j 3 , j 2 l 1 l 3 , j 1 l 2 l 3 1 , j 3 l 1 l 2 1 j 1 + j 2 l 1 l 2 , j 2 j 3 l 2 l 3 , j 1 j 3 l 1 l 3 1 ; 1 ) ,
2: 34.5 Basic Properties: 6 j Symbol
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 ) } ,
34.5.10 { j 1 j 2 j 3 l 1 l 2 l 3 } = { 1 2 ( j 2 + l 2 + j 3 l 3 ) 1 2 ( j 1 l 1 + j 3 + l 3 ) 1 2 ( j 1 + l 1 + j 2 l 2 ) 1 2 ( j 2 + l 2 j 3 + l 3 ) 1 2 ( j 1 + l 1 + j 3 + l 3 ) 1 2 ( j 1 + l 1 j 2 + l 2 ) } .
34.5.11 ( 2 j 1 + 1 ) ( ( J 3 + J 2 J 1 ) ( L 3 + L 2 J 1 ) 2 ( J 3 L 3 + J 2 L 2 J 1 L 1 ) ) { j 1 j 2 j 3 l 1 l 2 l 3 } = j 1 E ( j 1 + 1 ) { j 1 + 1 j 2 j 3 l 1 l 2 l 3 } + ( j 1 + 1 ) E ( j 1 ) { j 1 1 j 2 j 3 l 1 l 2 l 3 } ,
L r = l r ( l r + 1 ) ,
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 } .
3: B. L. J. Braaksma
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Boele L. J. Braaksma
Boele L. J. Braaksma (b. …
4: 25.15 Dirichlet L -functions
§25.15 Dirichlet L -functions
§25.15(i) Definitions and Basic Properties
The notation L ( s , χ ) was introduced by Dirichlet (1837) for the meromorphic continuation of the function defined by the series … …
§25.15(ii) Zeros
5: 20 Theta Functions
6: 14.30 Spherical and Spheroidal Harmonics
With l and m integers such that | m | l , and θ and ϕ angles such that 0 θ π , 0 ϕ 2 π , … Y l m ( θ , ϕ ) are known as surface harmonics of the first kind: tesseral for | m | < l and sectorial for | m | = l . Sometimes Y l , m ( θ , ϕ ) is denoted by i l 𝔇 l m ( θ , ϕ ) ; also the definition of Y l , m ( θ , ϕ ) can differ from (14.30.1), for example, by inclusion of a factor ( 1 ) m . … Here, in spherical coordinates, L 2 is the squared angular momentum operator: …and L z is the z component of the angular momentum operator
7: 34.8 Approximations for Large Parameters
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 ,
8: 18.39 Applications in the Physical Sciences
where L 2 is the (squared) angular momentum operator (14.30.12). The eigenfunctions of L 2 are the spherical harmonics Y l , m l ( θ , ϕ ) with eigenvalues 2 l ( l + 1 ) , each with degeneracy 2 l + 1 as m l = l , l + 1 , , l . … The functions ψ p , l ( r ) satisfy the equation, … The radial Coulomb wave functions R n , l ( r ) , solutions of … These, taken together with the infinite sets of bound states for each l , form complete sets. …
9: 22 Jacobian Elliptic Functions
10: Peter L. Walker
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Peter L. Walker
Peter L. Walker (b. …