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1: Software Index
Open Source With Book Commercial
25.21(ix) Dirichlet L -series a
  • 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.

  • 2: 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 ) ,
    3: 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 } .
    4: B. L. J. Braaksma
    Profile
    Boele L. J. Braaksma
    Boele L. J. Braaksma (b. …
    5: 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
    6: 20 Theta Functions
    7: 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
    8: 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 ,
    9: 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. …
    10: 22 Jacobian Elliptic Functions