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Figure 3
Double-crystal topograph of a quartz sample with induced growth striations, taken with a synchrotron double-crystal (n,−m) setup using a bendable perfect silicon monochromator [asymmetric 448 monochromator reflection (asymmetry angle α = −17.6°) in the Bragg case, FWHM of the exit beam after the monochromator 0.31″, 80 0 sample reflection (Bragg case) with FWHM = 0.07″, but now on the high-angle flank of the rocking curve, E = 17.7 keV]. The projection of the incident wavevector is indicated by k∣∣. |


journal menu![[Figure 3]](he0500fig3.jpg)
0 sample reflection (Bragg case) with FWHM = 0.07″, but now on the high-angle flank of the rocking curve, 


