Abstract
AbstractThe band corepresentations of the magnetic space groups are introduced; the procedure of their generation is considered. The band corepresentations are essential for the symmetry analysis of phonons and magnons in magnetic crystals and for the study of the magnon‐phonon hybridization. The magnetic structures of CuFeS2 and La2CuO4 crystals are analyzed. In the antiferromagnetic phase these crystals are described by Shubnikov space groups of different types. The band corepresentations for each of these groups are tabulated.
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