Abstract

The anisotropic spin exchange interactions of the magnetic solids CuM2O6 (M=Sb, V, Nb) were explained by analyzing their reported crystal structures and calculating the spin orbital interaction energies of their spin dimers. The magnetic orbital of each Cu2+ site in CuM2O6 is given by the “x2–y2” orbital so that the magnitude of an antiferromagnetic spin exchange interaction for a given spin dimer increases when the arrangement of the nearest-neighbor square-planar CuO4 units containing the magnetic orbitals provides a good sigma overlap between the adjacent magnetic orbitals. The one-dimensional magnetic chains of α-CuV2O6, β-CuNb2O6, and α-CuNb2O6 run along a direction different than their edge-sharing CuO4 chain directions. Our study predicts that the antiferromagnetic ordering in β-CuNb2O6 should make the magnetic unit cell double the chemical unit cell along the b-direction.

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