1993
DOI: 10.1016/0921-4526(93)90490-w
|View full text |Cite
|
Sign up to set email alerts
|

Surface and bulk electronic structure of metallic cerium systems

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

1995
1995
2003
2003

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 7 publications
(1 citation statement)
references
References 23 publications
0
1
0
Order By: Relevance
“…When we assume that this difference is due to the difference of the surface-to-bulk ratio, we may extract surface and bulk components from the two resonant spectra. 7,21 Providing that the surface contribution comes from the topmost Ce layer and the photoelectrons are emitted in the normal direction to the surface as expected from the present experimental setup, the surface-to-bulk emission ratio is given by exp(d/)Ϫ1, where d is the thickness of the surface layer and is the electron escape depth at a given kinetic energy. Using the formula for the electron escape depth by Tanuma, Powell, and Penn, 22 we obtain the values of for the 4d(3d)-4 f resonant spectra.…”
Section: Resultsmentioning
confidence: 86%
“…When we assume that this difference is due to the difference of the surface-to-bulk ratio, we may extract surface and bulk components from the two resonant spectra. 7,21 Providing that the surface contribution comes from the topmost Ce layer and the photoelectrons are emitted in the normal direction to the surface as expected from the present experimental setup, the surface-to-bulk emission ratio is given by exp(d/)Ϫ1, where d is the thickness of the surface layer and is the electron escape depth at a given kinetic energy. Using the formula for the electron escape depth by Tanuma, Powell, and Penn, 22 we obtain the values of for the 4d(3d)-4 f resonant spectra.…”
Section: Resultsmentioning
confidence: 86%