Abstract
Abstract The electronic structure of 1T-VS 2 and 1T-VSe 2 has been calculated using a non-spherical crystal potential. The widths of the various sub-band manifolds follow trends previously determined for other materials which crystallize in the CdI 2 structure. From the intrinsic Pauli paramagnetic susceptibility, we have derived a Stoner factor, effective exchange interaction and Coulomb pseudopotential. The density of states above E F is found to be in good agreement with that determined by Appearance Potential Spectroscopy. Additionally, the number of effective carriers has been derived and agrees to within 20% of that derived experimentally.
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