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The position (Formula presented) was chosen to reduce the contribution from the second harmonic (λ=0.062 nm) in the incident beam (which was passed by the (Formula presented) multilayer monochromator).
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The position (Formula presented) was chosen to reduce the contribution from the second harmonic (λ=0.062 nm) in the incident beam (which was passed by the (Formula presented) multilayer monochromator).
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25
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The herringbone pattern on Au(111) causes small changes in the spacings between layers near the surface and an increase in the atomic density in the top layer (Refs. 20, 21). Changes in the surface reconstruction during ion irradiation and homoepitaxy do not affect the qualitative conclusions drawn from the specular beam intensity measurements in Secs. IV and V. For the transverse x-ray scans through the (Formula presented) position reported in Secs. VI and VII, the influence of the reconstruction on the intensity is less than 1%.
-
The herringbone pattern on Au(111) causes small changes in the spacings between layers near the surface and an increase in the atomic density in the top layer (Refs. 20, 21). Changes in the surface reconstruction during ion irradiation and homoepitaxy do not affect the qualitative conclusions drawn from the specular beam intensity measurements in Secs. IV and V. For the transverse x-ray scans through the (Formula presented) position reported in Secs. VI and VII, the influence of the reconstruction on the intensity is less than 1%.
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The coverage of layers 0 (substrate), 1 and 2 after deposition of ≈1 ML in Ref. 15 indicate that the specular beam intensity at the anti-Bragg position after 1-ML deposition should be about 30–40% of the starting value.
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The coverage of layers 0 (substrate), 1 and 2 after deposition of ≈1 ML in Ref. 15 indicate that the specular beam intensity at the anti-Bragg position after 1-ML deposition should be about 30–40% of the starting value.
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