Abstract

The hyperfine properties of Mg such as Knight shift and electric field gradients (EFG) have been calculated from first principles as a function of temperature. The conduction-electron wave functions were obtained in the orthogonalized-plane-wave model by taking into account both the thermal expansion of the lattice and the effect of thermal vibrations of the ions on the crystal - field potential. The decrease in the ${p}_{x}\ensuremath{-}{p}_{y}$-like and ${p}_{z}$-like electrons with temperature leads to a decrease in the conduction-electron contribution to EFG. The lattice contribution is found to be rather insensitive to temperature and the conduction-electron part is largely responsible for the observed ${T}^{\frac{3}{2}}$ temperature dependence of the EFG. The decrease in the $p$ content of the wave function with temperature is accompanied by a simultaneous increase in the $d$ content and, to a small amount, of the $s$ content of the wave function. This small rise in the $s$-like electrons makes the Knight shift less dependent upon temperature than the EFG---an observation consistent with experimental data.

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