1983
DOI: 10.1107/s002188988301047x
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On the X-ray reflectivity of elastically bent perfect crystals

Abstract: The integrated X-ray reflectivity of elastically bent, but otherwise perfect, crystals are calculated for Lauetype reflections covering the entire curvature range. Anomalous transmission and elastic anisotropy are taken into account, and it is shown that both these effects affect appreciably the reflected intensities for both weakly and strongly bent crystals. The validity of the reflectivity-versus-curvature relation thus obtained is experimentally confirmed for a number of reflections from silicon crystals. … Show more

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Cited by 23 publications
(22 citation statements)
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“…Diffracting planes may be expected to have a mean angle 0~plan e with respect to the surface for flat or curved crystals. Use of a constant %ta,e assumes either that materials are isotropic or that %~ane is small, but is generally the first-order contribution (el Kalman & Weissman, 1983). Then,…”
Section: Allowance For Depth Penetration and Johann Geometrymentioning
confidence: 99%
“…Diffracting planes may be expected to have a mean angle 0~plan e with respect to the surface for flat or curved crystals. Use of a constant %ta,e assumes either that materials are isotropic or that %~ane is small, but is generally the first-order contribution (el Kalman & Weissman, 1983). Then,…”
Section: Allowance For Depth Penetration and Johann Geometrymentioning
confidence: 99%
“…5 Many methods to model the diffraction profiles of bent crystals have been developed and implemented in the XCRYSTAL BENT module 6 of the XOP package. 7 The multi-lamellar (ML) approximation [8][9][10][11] and the Penning-Polder (PP) method [12][13][14][15] both provide reasonable results in the case of crystals bent cylindrically in the diffraction plane. However, the applications of these theories to simulate the rocking curves of sagittally bent crystals are not yet studied in detail.…”
Section: Introductionmentioning
confidence: 98%
“…A lamellar model has been used successfully in both the Bragg and Laue geometries to explain X-ray and neutron diffraction by such crystals (Egert & Dachs, 1970;Albertini et al, 1976;Boeuf et al, 1978;Mikula et al, 1984). Similar treatments were worked out for meridionally bent anisotropic crystals (Kalman & Weissmann, 1983;. Theories have been derived for the angular acceptance of meridionally bent isotropic crystals (Caciuffo et al, 1987;Popovici et al, 1988;Erola et al, 1990;Hiraoka et al, 2001).…”
Section: Introductionmentioning
confidence: 99%
“…From results obtained for plates of constant cross section bent by equal but opposite moments, the displacement ®eld is (Voigt, 1928;Kalman & Weissmann, 1983;Chukhovskii et al, 1994) u x Ex 2 S 13 À y 2 S 23 À zyS 43 À z 2 S 33 u y Ex 2 S 63 2xyS 23 xzS 43 1 u z Ex 2 S 53 xyS 43 2xzS 33 Y where S ij are the elastic compliances of the crystal for a speci®c orientation, u xYyYz are displacements in the x, y and z directions, respectively, and E is a constant related to the bending moment and moment of inertia of the crystal. Thus, it is necessary to take into consideration the anisotropy of the crystal.…”
Section: Introductionmentioning
confidence: 99%