2000
DOI: 10.1002/1521-396x(200005)179:1<103::aid-pssa103>3.0.co;2-i
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Experimental Observation of X-Ray Diffraction from a Thin Crystalline Film at a 90� Bragg Reflection

Abstract: The first experimental observation of diffraction from a thin surface layer at a 90 Bragg reflection is reported. A thin (< 1 mm) InGaAs film deposited on a GaAs(800) substrate was studied near the 90 Bragg position. Slight, less than 0.1%, difference in the lattice spacing between the layer and the substrate, has allowed, for the first time, a direct and exclusive observation of the diffraction profile from a thin layer as if it was a ªfree-standingº thin crystal.

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Cited by 6 publications
(4 citation statements)
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“…A use of semitransparent crystalline detectors such as p-i-n or avalanche photodiodes would very likely lead to unpredictable parasitic reflections inside such detectors. 15 The two-dimensional (angle-energy) intensity profiles in the vicinity of the exact 90°Bragg reflection position were collected as a function of the angular position of the crystal sample and incident synchrotron x-ray energy. The x-ray energy was selected by the primary beamline monochromator with consecutive realignment of the second monochromator to ensure the optimal mutual position of these two crystals along the optical axis.…”
Section: Methodsmentioning
confidence: 99%
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“…A use of semitransparent crystalline detectors such as p-i-n or avalanche photodiodes would very likely lead to unpredictable parasitic reflections inside such detectors. 15 The two-dimensional (angle-energy) intensity profiles in the vicinity of the exact 90°Bragg reflection position were collected as a function of the angular position of the crystal sample and incident synchrotron x-ray energy. The x-ray energy was selected by the primary beamline monochromator with consecutive realignment of the second monochromator to ensure the optimal mutual position of these two crystals along the optical axis.…”
Section: Methodsmentioning
confidence: 99%
“…Thus, Eqs. (15) and (20) form a system that can be solved with respect to unknown coefficients c ͑n͒ . Using the recurrence formula (20), the final relation between c ͑1͒ and c ͑N͒ can be written as…”
Section: ͑19͒mentioning
confidence: 99%
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