Numéro |
J. Phys. IV France
Volume 7, Numéro C2, Avril 1997
Proceedings of the 9th International Conference on X-Ray Absorption Fine Structure
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Page(s) | C2-251 - C2-252 | |
DOI | https://doi.org/10.1051/jp4/1997186 |
J. Phys. IV France 7 (1997) C2-251-C2-252
DOI: 10.1051/jp4/1997186
Effective Coordination Numbers in Ultrathin Metallic Films
E.D. Crozier, A.J. Seary, M.K. McManus and D.T. JiangDepartment of Physics, Simon Fraser University, Burnaby, BC Canada V5A 1S6
Abstract
Nanostructures bave become a major field in material science. With molecular beam epitaxy it is possible to engineer
multilayers with unusual anisotropic properties and metastable structures. For ultrathin films, or particles of small size, the
coordination numbers are less than their bulk values. In fitting E X A F S data it is useful to be able to place limits on the
coordination numbers or their ratios. W e have calculated the effective coordination numbers Ni , i= 1 to 5 for thin films with
different crystal structures. The thickness o f the film is specified by the number o f layers Nz in the z-direction and the area in
the x y plane by the number o f rows of atoms NXY along the side of a square domain. For fixed Nz, with the x-ray beam
unpolarized or its electric vector parallel or perpendicular to the substrate (xy plane), the effective H approach hyperbolically
the coordination number for a layer o f infinite area. Simple analytical expressions are fitted to the numerical results fix- bcc and
fee crystals from which the H can be calculated for both NXY and Nz ≥ 2. Comparison is made with the effective coordination
numbers obtained from polarized E X A F S measurements on epitaxial metallic films less than 10 monolayers thick.
© EDP Sciences 1997