Abstract
Electron–positron momentum densities in CuCl are calculated along two different crystallographic directions 〈001〉 and 〈110〉 with the use of the empirical pseudopotential method (EPM) coupled with the independent particle method (IPM). The results exhibit features that are completely different from those observed in other III–V semiconductors. The dip and valley observed in III–V compounds are replaced by peaks. These differences are attributed to the very shallow “d” states in copper.
Sign-in/Register to access full text options 
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 callDisclaimer: 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.
