Physics – Condensed Matter – Materials Science
Scientific paper
2001-03-22
Phys. Rev. B 66, (2002) 045402
Physics
Condensed Matter
Materials Science
1 new figure, updated references; to be published in Phys. Rev. B
Scientific paper
10.1103/PhysRevB.66.045402
A few theoretical models predict Fe to display both ferromagnetic and antiferromagnetic phases, depending on the volume of the unit cell. A proper choice of the substrate allows the growth of thin Fe overlayers with structures different from the bcc bulk one. The Cu3Au(001) substrate is a suitable candidate for testing these magnetic properties since it has a lattice parameter (3.75 Angstroms) which lies closer to the ferromagnetic fcc Fe phase (3.66 Angstroms) than to the ferromagnetic bcc phase (4.07 Angstroms). We have investigated Fe films up to 40 Angstroms thickness by means of Grazing Incidence X-Ray Diffraction (GIXRD) and Photo/Auger--Electron Diffraction (ED). The combination of GIXRD and ED allows one to obtain quantitative information on the in--plane spacing "a" from the former technique, and the ratio between the vertical spacing "c" and "a", from the latter one. At low coverage the film grows pseudomorphic to the fcc substrate up to a limit thickness of 8 Angstroms. Above this limit the film is characterized by the coexistence of the pseudomorphic phase with another tetragonally strained phase. The latter phase is shown to fall on the epitaxial curve of tetragonally distorted fcc Fe phase. Finally, above 17 Angstroms the development of a body centered phase "alpha", whose unit cell is rotated of 45 deg. with respect to the substrate one, has been clearly observed. "alpha" is the dominating phase for film thickness higher than 25 Angstroms and its lattice constant evolves towards the orthomorphic phase in strict quantitative agreement with epitaxial curves calculated for the tetragonally distorted bcc iron phase.
Bruno Fabre
Canepa M.
Cossaro A.
Cvetko Dean
Floreano L.
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