Experimental determination of the instrumental transparency function of texture goniometers

Citation
K. Moras et al., Experimental determination of the instrumental transparency function of texture goniometers, J APPL CRYS, 33, 2000, pp. 1162-1174
Citations number
13
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF APPLIED CRYSTALLOGRAPHY
ISSN journal
00218898 → ACNP
Volume
33
Year of publication
2000
Part
4
Pages
1162 - 1174
Database
ISI
SICI code
0021-8898(20000801)33:<1162:EDOTIT>2.0.ZU;2-R
Abstract
The instrumental transparency functions of five commercially available text ure goniometers were measured experimentally with six monocrystalline sampl es cut in different orientations from a large highly perfect silicon crysta l with a rocking curve of less than 0.01 degrees. Transparency functions we re measured in steps of 0.02 to 0.2 degrees in the pole-figure angles alpha , beta. The window size Delta alpha depends on the Bragg angle theta in the form 1/sin theta; the window size Delta omega is constant for each goniome ter. The dominant instrumental parameter determining the long axis Delta al pha of the pole-figure window is the axial width of the detector entrance s lit. This parameter is smallest for area detectors (smaller by more than an order of magnitude compared with conventional scintillation detectors as w ell as one-dimensional position-sensitive detectors). The main features of the pole-figure window and their dependence on the instrumental parameters can be deduced fairly well from a simple geometrical model. The particular shapes of the transparency functions of the studied goniometers are markedl y different. Particularly, they are not very well represented by Gauss func tions. The two-dimensional transparency function can be fairly well charact erized by its alpha and beta profiles. The normalized profiles are virtuall y independent of the goniometer angles 2 theta and alpha. The increasing si ze of the pole-figure window with decreasing theta puts a lower limit on th e Bragg angle below which pole-figure measurement ceases to be meaningful.