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Multiplets with magnetic angular momentum

The zero-order energy accounting for the equivalence coefficients adopts the form of [Pg.482]

It leads to the following zero-order van Vleck coefficient [Pg.482]

The first-order perturbation correction to the energy is given by the electronic Zeeman term as follows [Pg.483]

M) = VLBBzgyj[jM jz jM)[r ] = iiBBzgYjM yields the Lande factor modified to the form [Pg.483]

Consequently the first-order van Vleck coefficients become [Pg.483]


See other pages where Multiplets with magnetic angular momentum is mentioned: [Pg.482]    [Pg.482]    [Pg.100]    [Pg.11]    [Pg.191]    [Pg.283]    [Pg.197]    [Pg.200]    [Pg.248]    [Pg.250]    [Pg.254]    [Pg.258]    [Pg.4]    [Pg.40]    [Pg.583]    [Pg.1396]    [Pg.201]    [Pg.334]    [Pg.105]    [Pg.353]    [Pg.5]    [Pg.5]    [Pg.349]    [Pg.356]    [Pg.262]    [Pg.158]    [Pg.669]    [Pg.97]   


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