2018
DOI: 10.1107/s2053273318012627
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Computer simulations of X-ray spherical wave dynamical diffraction in one and two crystals in the Laue case

Abstract: This article reports computer simulations of X‐ray spherical wave dynamical diffraction in one and two single crystals in the Laue case. An X‐ray compound refractive lens (CRL) as a secondary radiation source of spherical waves was considered for the first time and in contrast to previous simulations with the assumption of the use of a slit. The main properties of the CRL as a secondary source are discussed and two focusing phenomena are analysed. The first one is the diffraction focusing effect for one single… Show more

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Cited by 4 publications
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“…The average reflected-beam intensity at the lower boundary (i.e., at the thickness t 1 ) is assumed to be unity. Note that the diffraction-focusing thickness [12,36] for the distance under consideration is t df = L|χ h |F = 60.8 μm, where F = 1/(sin θ B sin 2θ B ). Therefore, a part of radiation with weak absorption is maximally compressed at this thickness, then it diverges again, and exhibits an almost uniform intensity distribution over the x axis (along the surface) in the step region.…”
Section: Resultsmentioning
confidence: 99%
“…The average reflected-beam intensity at the lower boundary (i.e., at the thickness t 1 ) is assumed to be unity. Note that the diffraction-focusing thickness [12,36] for the distance under consideration is t df = L|χ h |F = 60.8 μm, where F = 1/(sin θ B sin 2θ B ). Therefore, a part of radiation with weak absorption is maximally compressed at this thickness, then it diverges again, and exhibits an almost uniform intensity distribution over the x axis (along the surface) in the step region.…”
Section: Resultsmentioning
confidence: 99%