Abstract:Some characteristics are reported of a triple-crystal diffractometer with a (+, −, +) setting of Si(220) using mirage diffraction. The first crystal is flat, while the second and third crystals are bent. Basically, the first crystal is used as a collimator, the second as a monochromator and the third as the sample. The third crystal also works as an analyzer. The advantages of this diffractometer are that its setup is easy, its structure is simple, the divergence angle from the second crystal is small and the … Show more
“…In order to observe mirage interference fringes, a finite divergence angle Á is needed. The divergence angle Á is related to the divergence angle Á B of the beam from the monochromator as jÁ B j ¼ sin 2 B jÁj ð 41Þ (Fukamachi et al, 2014(Fukamachi et al, , 2015(Fukamachi et al, , 2019. By using the Bragg condition, the width ÁE of X-ray energy (E) and the angle width Á B are related as…”
The dynamical theory of diffraction is used to analyse irregular X-ray mirage interference fringes observed in Si220 X-ray reflection topography from a weakly bent, thin crystal due to gravity. The origin of the irregular fringes is attributed to the interference between mirage diffracted beams and a reflected beam from the back surface, which is a new type of interference fringe. The irregular fringes are reproduced by calculating the reflected intensities numerically. The effects of absorption and thermal vibration are quite important for the reproduction. The result shows that the interference fringes depend on the strain as well as the thickness of the crystal, which indicates that the fringes should be useful for analysing weak strain in a crystal as an application.
“…In order to observe mirage interference fringes, a finite divergence angle Á is needed. The divergence angle Á is related to the divergence angle Á B of the beam from the monochromator as jÁ B j ¼ sin 2 B jÁj ð 41Þ (Fukamachi et al, 2014(Fukamachi et al, , 2015(Fukamachi et al, , 2019. By using the Bragg condition, the width ÁE of X-ray energy (E) and the angle width Á B are related as…”
The dynamical theory of diffraction is used to analyse irregular X-ray mirage interference fringes observed in Si220 X-ray reflection topography from a weakly bent, thin crystal due to gravity. The origin of the irregular fringes is attributed to the interference between mirage diffracted beams and a reflected beam from the back surface, which is a new type of interference fringe. The irregular fringes are reproduced by calculating the reflected intensities numerically. The effects of absorption and thermal vibration are quite important for the reproduction. The result shows that the interference fringes depend on the strain as well as the thickness of the crystal, which indicates that the fringes should be useful for analysing weak strain in a crystal as an application.
“…In the experiment, the incident glancing angle () is fixed and the X-ray from the bending magnet is a wave having an energy spread of E and the corresponding deviation of wavenumber jK E j. The divergent angle of the X-ray at the incident point on the crystal surface is related to the energy width E, as discussed by Fukamachi et al (2014Fukamachi et al ( , 2015.…”
Section: Coherent Condition and Energy Width Of Ifrbmentioning
confidence: 99%
“…For simplicity, the glancing angle is assumed to be the same as B . The dispersion surfaces and the diffraction geometry in the more general case are given by Fukamachi et al (2014Fukamachi et al ( , 2015. The vector OH !…”
In the waves emitted from the entrance, back and lateral surfaces of a very weakly bent plane-parallel perfect crystal with negative strain gradient, X-ray interference fringes between two refracted beams with different hyperbolic trajectories were observed when the strain was very weak, of the order of 10−7.
“…As the last sentence of the caption of Fig. 2 of Fukamachi et al (2014), the following sentence should be added: jK E j is the distance between a 2 and a 4 . Fig.…”
mentioning
confidence: 99%
“…Fig. 2 of Fukamachi et al (2014) is updated as Fig. 1 in the current article to reflect the correction.…”
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