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IGCAR : Annual Report - Indira Gandhi Centre for Atomic Research

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IGC<br />

<strong>Annual</strong> <strong>Report</strong> 2007<br />

characterization of the crystals<br />

and even today it is the first step<br />

in assessing the crystal quality.<br />

In the Laue camera, instead of<br />

the photographic X-ray film an<br />

imaging plate cut in a circular<br />

shape is loaded and covered<br />

with an opaque paper. The<br />

exposed plates are scanned to<br />

obtain the image. The Laue<br />

diffraction pattern <strong>for</strong> Si crystal<br />

in both transmitted and back<br />

reflected geometries are given<br />

in Fig.1. The inset in Fig. 1<br />

shows the enlarged view of a<br />

particular Laue spot which<br />

depends on the nature of the<br />

crystal.<br />

The powder XRD experiment<br />

was carried out using the<br />

imaging plate <strong>for</strong> a BaF 2<br />

standard sample. The sample<br />

was kept in front of the<br />

collimator in Debye Scherrer<br />

geometry and the imaging plate<br />

kept at a distance of 77.6 mm<br />

from the sample. Mo K X-ray<br />

°<br />

with a wavelength of 0.709 A is<br />

used <strong>for</strong> this experiment. The<br />

Fig.2 Powder diffraction pattern of BaF 2 sample; with some isolated<br />

diffraction spots along the Debye rings indicated using the small circles<br />

in the images. The blue circle and the arc shows the psi angle<br />

XRD image obtained is shown<br />

in figure 2. The sample was<br />

well powdered be<strong>for</strong>e carrying<br />

out the diffraction experiment.<br />

In spite of this there are a few<br />

isolated diffraction spots<br />

(shown by the circles in the<br />

image) in the powder pattern<br />

indicating the coarse grained<br />

nature of the sample. This 2D<br />

pattern is converted into a 1D<br />

pattern by azimuthal integration<br />

of pixel intensities from 0 to<br />

360° and by increasing the<br />

radius value from the centre of<br />

the concentric rings to the edge<br />

of the plate (2000 units). The<br />

center point of the rings is<br />

identified by triangulation of<br />

Fig.2 Powder diffraction pattern of BaF 2 sample; with some isolated<br />

diffraction spots along the Debye rings indicated using the small circles<br />

in the images. The blue circle and the arc shows the psi angle<br />

three points of any one of the<br />

rings. This centre is a crucial<br />

factor in the 1D data quality<br />

hence its accurate location is<br />

essential. In order to compare<br />

the integrated data with that<br />

collected using a standard<br />

powder diffractometer (with a<br />

point detector), the intensity of<br />

every 2 step is normalized by<br />

the number of pixels<br />

contributing to it. Also in the<br />

converted data there is high<br />

background hence it is<br />

removed from the image using<br />

an algorithm. The as acquired<br />

XRD image and the background<br />

subtracted image are shown in<br />

Fig. 2 and the inset (intensity<br />

plot along the circumference of<br />

the ring) shows the coarse<br />

grained nature in the sample.<br />

The converted 1D pattern<br />

be<strong>for</strong>e and after removing the<br />

background is shown in figure<br />

3. The conclusion is that if<br />

there is a single crystal<br />

diffractometer with area<br />

detector like imaging plate the<br />

same could be used <strong>for</strong> powder<br />

diffraction experiments.<br />

BASIC RESEARCH 167

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