Abstract

In a system of concentrated $4f$ ions with two configurations $4{f}^{n}$ and $4{f}^{n\ensuremath{-}1}$ competing for stability, a narrow resonance in the electronic density of states near the Fermi energy is expected. Using an explicitly configuration-based approach with appropriate intraconfigurational splittings included, we obtain a sum rule on the integrated density of states and a microscopic estimate of the resonance width. The width, identifiable with an interconfiguration fluctuation rate, is proportional to the nominal mixing width $\ensuremath{\Delta}({\ensuremath{\epsilon}}_{F})=\ensuremath{\pi}{|{V}_{\mathrm{mix}}|}^{2}{\ensuremath{\rho}}_{\mathrm{cond}}({\ensuremath{\epsilon}}_{F})$, but with a proportionality factor depending rather strongly upon the specific ionic states involved. Results are obtained for electronic specific heats, x-ray photoemission linewidths, and M\"ossbauer spectra in such systems.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.