Effects of elastic-electron scattering on measurements of silicon dioxide film thicknesses by X-ray photoelectron spectroscopy

Citation
Cj. Powell et A. Jablonski, Effects of elastic-electron scattering on measurements of silicon dioxide film thicknesses by X-ray photoelectron spectroscopy, J ELEC SPEC, 114, 2001, pp. 1139-1143
Citations number
14
Categorie Soggetti
Spectroscopy /Instrumentation/Analytical Sciences
Journal title
JOURNAL OF ELECTRON SPECTROSCOPY AND RELATED PHENOMENA
ISSN journal
03682048 → ACNP
Volume
114
Year of publication
2001
Pages
1139 - 1143
Database
ISI
SICI code
0368-2048(200103)114:<1139:EOESOM>2.0.ZU;2-P
Abstract
It is now customary for the effects of elastic-electron scattering to be ig nored in measurements of the thicknesses of overlayer films by X-ray photoe lectron spectroscopy (XPS). It is known, however, that elastic scattering c an cause the effective attenuation length (EAL), needed for the thickness m easurement, to be different from the corresponding inelastic mean free path (IMFP). We have investigated the effects of elastic-electron scattering in measurements of thicknesses of SiO2 films on Si from XPS measurements with Al and Mg K alpha X-rays. Calculations were made of substrate and oxide Si 2p photoelectron currents for different oxide thicknesses and emission ang les using an algorithm based on the transport approximation. This algorithm accounts for the occurrence of elastic scattering along electron trajector ies in the solid. The calculations simulated an angle-resolved XPS experime nt in which the angle psi between the X-ray source and the analyzer axis wa s 40 degrees, 54 degrees, or 70 degrees. For each SiO2 thickness and set of measurement conditions, an average EAL was determined from the substrate c urrents with and without the oxide overlayer. The ratio of the average EAL to the IMFP varied with SiO2 thickness, emission angle alpha, the angle psi ; and the X-ray energy. For alpha less than or equal to 65 degrees and for oxide thicknesses such that the substrate current was reduced to not less t han 10% of its original value, the mean EAL for this range of thicknesses w as between 0.912 and 0.926 of the corresponding IMFP for Mg K alpha X-rays (for the three psi values) and between 0.922 and 0.935 for Al K alpha X-ray s. For larger emission angles, the ratio of the mean EAL to the IMFP varied considerably with alpha and psi An EAL value appropriate for the measureme nt conditions should be chosen for measurements of SiO, thicknesses by XPS. (C) 2001 Elsevier Science B.V. All rights reserved.