Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
5426141 | Surface Science | 2007 | 12 Pages |
We investigated the growth of Fe nanostructured films on c(2 Ã 2)-N/Cu(1 0 0) surface with Fe K-edge X-ray absorption fine structure (XAFS) in the near edge and in the extended energy region. The high photon flux of the incident X-rays allowed us to perform multishell analysis of the XAFS oscillations for Fe coverage ÎFe < 1 ML. This data analysis yields a detailed investigation of the atom geometry and some insights in the film morphology. At ÎN < 0.5 ML (N saturation coverage) there is absence of contribution to XAFS from N atoms. First shell analysis of linearly polarized XAFS gives Fe-Fe (or Fe-Cu) bond length values varying between R1 = 2.526 ± 0.006 à at the highest Fe coverage (3 ML ) and R1 = 2.58 ± 0.01 à at ÎFe = 0.5 ML, ÎN = 0.3 ML, with incidence angle Π= 35°. These values are different from the case of bcc Fe (R = 2.48 à ), and compatible with fcc Fe (R1 = 2.52 à ) and fcc Cu (R1 = 2.55 à ). At the Fe lowest coverage (ÎFe = 0.5 ML) the dependence of R1 on the incidence angle indicates expansion of the outmost layer. Near edge spectra and multishell analysis can be well reproduced by fcc geometry with high degree of static disorder. At N saturation pre-coverage (ÎN = 0.5 ML) the XAFS analysis has to keep into account the Fe-N bonding. The results suggest two different adsorption sites: one with Fe in a fcc hollow site, surrounded by other metal atoms as nearest neighbours, and one resulting from an exchange with a Cu atom underneath the N layer.