The results of a relativistic tight-binding energy-band model for Pt and Au, utilizing parameters derived from Smith's empirically adjusted combined interpolation scheme, are applied to calculate the one-electron contribution to various x-ray and energy-loss spectra involving $4f$ and $2p$ core states in these materials. These results show that the unoccupied holes in the Pt $5d$ bands have predominantly j=5/2 character (h5/2) such that the (h5/2h3/2) ratio ranges from {~}3.5 within 0.5 eV of EF to {~}2.9 over the entire unoccupied conduction band. Taking into account dipole transition probabilities, the former ratio leads to a predicted line-strength ratio I_N₇I_N₆≈2.9 near threshold for excitations involving the $4f$$j=7/2({N}₇)$ and $j=5/2({N}₆)$ core levels in Pt. This result is in good agreement with the corresponding experimental ratios that are derived from electron energy-loss (2.5) and x-ray-absorption (2.3) spectra. Comparable agreement is obtained between the calculated and observed (electron-energy-loss) I_N₇I_N₆ ratios in Au. The present results are applied to calculate the N₆-N₇ x-ray emission spectra in both Pt and Au and to interpret the L₂-L₃ absorption-edge data in Pt.
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Mattheiss et al. (1980) studied this question.
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