Abstract
The fine structure (FS) of the experimental secondary electron emission spectra (SEES) along the normal to Ir(111) surface and the target (total) current spectra (TCS) of Cu(111) surface are interpreted theoretically. It is shown that the FS of SEES and TCS is mainly due to the electronic structure of finite states to which the electrons come or from which they emit. The predominant role of the effects of bulk energy-band structure in the formation of spectra is shown.
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.
