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Clebsch-Gordan coefficients symmetry relations

For a given j, we may also consider the case with an orbital angular momentum quantum number V larger than j so that j = I — (thus, Z = Z + 1 if j shall adopt the same value as before). However, for j = 1 — and V > 0, we cannot exploit Eq. (4.142) directly, but need to rearrange the Clebsch-Gordan coefficient first so that the constraint for Eq. (4.142), J = ji + )2, is fulfilled. From well-known symmetry relations for Clebsch-Gordan coefficients [75] we find... [Pg.151]

Usine symmetry relations, Clebsch-Gordan coefficients... [Pg.2652]


See other pages where Clebsch-Gordan coefficients symmetry relations is mentioned: [Pg.31]    [Pg.2523]    [Pg.2679]    [Pg.739]    [Pg.2304]    [Pg.2628]    [Pg.2648]    [Pg.147]    [Pg.2458]   
See also in sourсe #XX -- [ Pg.274 ]




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