Hb. Neumann et al., THE RESOLUTION FUNCTION OF A TRIPLE-CRYSTAL DIFFRACTOMETER FOR HIGH-ENERGY SYNCHROTRON-RADIATION IN NONDISPERSIVE LAUE GEOMETRY, Journal of applied crystallography, 27, 1994, pp. 1030-1038
The k-space resolution function of a triple-crystal diffractometer is
calculated for an arrangement of three perfect silicon single crystals
Bragg diffracting in nondispersive Laue geometry. A comparison is mad
e with the results of measurements using synchrotron radiation in the
energy range from 80 to 150 keV. In this case, absorption is very weak
and according to dynamical theory the width of the diffraction patter
n of thick perfect single crystals is proportional to the wavelength l
ambda, whereas its Lorentzian tails are proportional to lambda(2). Tog
ether with the fact that the Bragg angles are only of the order of 2 d
egrees, this leads to a concentration of the starlike k-space resoluti
on function into a narrow band parallel to the reciprocal-lattice vect
or G. For diffraction of 80 keV synchrotron radiation at the silicon 1
11 reflection, the full width at half-maximum (FWHM) of the intensity
distribution in the scattering plane is 1.1 x 10(-5) Angstrom(-1) perp
endicular to G and 2.2 x 10(-4) Angstrom(-1) parallel to G. The observ
ed differences in the contributions from monochromator and analyzer cr
ystal to the resolution function are explained by the finite width of
the electronic window of the detector counting chain and the non-Bragg
scattering contribution from the crystals. If annealed Czochralski-gr
own silicon single crystals with a mosaicity of similar to 3'' are use
d as monochromator and analyzer, the resolution is reduced by one orde
r of magnitude, but for studies of imperfect samples or of diffuse sca
ttering large gains in intensity can be accomplished this way.