Abstract
It is shown that recent measurements of field ion energy distributions from clean tungsten surfaces probe the density of metal states in the vicinity of the surface. We find j( ω) = (2 π/ kh) Σ m | ∫ d 3 rψ m ( r) γ z | 2 δ( ω− ϵ m ), where j(ω) is the ion current a ω, ψ m and ϵ m are electronic metal eigenfunctions and eigenvalues in the presence of the external electric field used in field ionization and γ( z) is a function which is large near the noble gas atom. An explicit expression for γ( z) is given in the text. It is estimated that tungsten metal states with values of k ‖ at least as large as 0.5 Å −1 make an appreciable contribution to j(ω) where k ‖ is the electron momentum parallel to the surface.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
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.