Abstract
The K emission band spectra of 3d metals were measured with a two-crystal spectrometer. The total and partial densities of states and the K emission spectra were computed from the band structure calculation. Good overall agreement between theory and experiment is obtained. The longstanding discrepancy in the FWHM in Ni K and Fe K bands was removed by using a linear energy dependence suggested recently for Auger broadening. The systematic changes in the structures of the spectra can be explained by the present theory based on the one-electron description and dipole approximation. The results for V, Fe, Ni and Cu are presented here.
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