Electronic and magnetic structure of thin Ni films on Co/Cu(001)

Citation
Ss. Dhesi et al., Electronic and magnetic structure of thin Ni films on Co/Cu(001), PHYS REV B, 60(18), 1999, pp. 12852-12860
Citations number
43
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B-CONDENSED MATTER
ISSN journal
01631829 → ACNP
Volume
60
Issue
18
Year of publication
1999
Pages
12852 - 12860
Database
ISI
SICI code
0163-1829(19991101)60:18<12852:EAMSOT>2.0.ZU;2-X
Abstract
The electronic and magnetic structure of ferromagnetic Ni films grown epita xially on ultrathin Films of Co has been studied by x-ray-absorption spectr oscopy (XAS) using circular polarization. The growth morphology of the film s was verified using high-resolution low-energy electron diffraction and in dicated an incomplete layer-by-layer growth mode for the Co and Ni films de posited on Cu(001). We report the presence of additional peaks in the x-ray magnetic circular dichroism (XMCD) as predicted by the configuration inter action model. The ground-state magnetic moments were obtained from the XMCD sum rules at the Ni 2p edge. For a film thickness below 2 ML the number of holes and the spin polarization (spin moment per hole) show a gradual decr ease, while the orbital polarization (orbital moment per hole) and the spin -orbit interaction show a gradual increase in magnitude. The 6-eV satellite structure, which is present in the XAS and XMCD of bulk Ni, disappears for submonolayer coverages while the dichroism due to "diffuse magnetism" betw een the L-3 and L-3 edges is strongly enhanced. These observations are ascr ibed to changes in the hybridization (electronic mu;mg) as a function of fi lm thickness, which influences the ground-state d(8) weight and the s-state spin polarization. The strongly increased orbital moment per spin provides a good measure for the degree of localization. It is shown that for Ni thi n firms a localization of the wave function does not lead to an enhancement in the total magnetic moment, but, on the contrary, its value is twice as small as the bulk value. [S0163-1829(99)0521 1-8].