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The measurements were carried out with He+ ions of 1 MeV at the Dynamitron in Stuttgart. The RBS-chamber has an IBM-geometry (i.e., the detector is located at θ = 165° scattering angle in the same plane as the beam and the sample normal) with a detector resolution of 14 keV.
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x in Fig. 2(a) shows oscillations which do not correspond to the thickness oscillations of a 5800 Å thick aluminum oxide film. During preparation of this specific film the sputtering process was interrupted to cool down the sputtering target. After restarting sputtering the preparation conditions might have changed slightly. The reflectivity curve could be fitted using a model with two aluminum oxide films of slightly different electron density but total film thickness of ca. 5800 Å.
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x in Fig. 2(a) shows oscillations which do not correspond to the thickness oscillations of a 5800 Å thick aluminum oxide film. During preparation of this specific film the sputtering process was interrupted to cool down the sputtering target. After restarting sputtering the preparation conditions might have changed slightly. The reflectivity curve could be fitted using a model with two aluminum oxide films of slightly different electron density but total film thickness of ca. 5800 Å.
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We note that this β values arise under the present specific sputtering conditions employed in this study, but is not necessarily universal. We rather expect it to change with sputtering power, geometry, argon gas pressure and other experimental parameters.
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We note that this β values arise under the present specific sputtering conditions employed in this study, but is not necessarily universal. We rather expect it to change with sputtering power, geometry, argon gas pressure and other experimental parameters.
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