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Unitary group irreps

We assume that the canonical orbitals 95m (k,r) = (pbasis vectors of irrep 7 with wavevector k, n discriminates between the independent bases of equivalent irreps the index a replaces 7, m,ij, and s replaces a, k) of an energy band under consideration form a basis in the space < (q,/3) of some indrep of the group G > of a crystal. The localized functions are defined by a unitary transformation in the space of indrep ... [Pg.96]

It remains to discuss case 1, where both functions in a Kramers pair belong to the same irrep. For this case, ordinary point group symmetry does not promise any a priori blocking. We will therefore look for a unitary transformation on the Kramers pair basis that can block-diagonalize a matrix constructed over functions belonging to a case 1 irrep. The problem can be reduced to the diagonalization of a general 2x2 matrix spanned by the components of a Kramers pair. For the operator this is... [Pg.153]


See other pages where Unitary group irreps is mentioned: [Pg.34]    [Pg.13]    [Pg.229]    [Pg.31]    [Pg.109]    [Pg.334]    [Pg.559]    [Pg.667]    [Pg.97]    [Pg.41]    [Pg.9]    [Pg.667]    [Pg.58]    [Pg.50]   
See also in sourсe #XX -- [ Pg.334 , Pg.337 , Pg.338 ]




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