1977
DOI: 10.1107/s0567739477001090
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Dynamical contrast of the topographic image of a crystal with continuous X-ray radiation. II. A theoretical study of the polychromatic interference fringes

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Cited by 26 publications
(3 citation statements)
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“…This is impossible for beams The geometry of the experiment was in accordance with Fig. 1 (z 1 = 100-150 mm, z 3 = 50-300 mm) and was very similar to that of Aristov, Shmytko & Shulakov (1977b). In order to decrease the background of radiation scattered by various elements of the experimental scheme the primary beam divergence was limited to 4-6 o by slit 1.…”
Section: Resultsmentioning
confidence: 99%
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“…This is impossible for beams The geometry of the experiment was in accordance with Fig. 1 (z 1 = 100-150 mm, z 3 = 50-300 mm) and was very similar to that of Aristov, Shmytko & Shulakov (1977b). In order to decrease the background of radiation scattered by various elements of the experimental scheme the primary beam divergence was limited to 4-6 o by slit 1.…”
Section: Resultsmentioning
confidence: 99%
“…The range of wavelengths contributing to the total intensity at the observation point is determined by the width of the monochromatic beams (2Ttan era/cos ~'), the interferometer defocusing (zlb = b 2 --b~) (usually,, and the experimental geometry. It may be considered that only those rays are incident upon the point r e for which the following condition is fulfilled (Aristov et al, 1977a):…”
Section: Ismentioning
confidence: 99%
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