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Neutron Scattering

Neutron Scattering - JuSER - Forschungszentrum Jülich

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Fig. 18.14: Variation of reflection<br />

intensities ivith rp rotation (x<br />

f'xed) ofa quartzit sample<br />

measured ivith a large linear<br />

detector in Jülich<br />

Rather than using a single counfng tube it is more efficient to employ a large positionsensitive<br />

detector which covers a wide scattering range 20 and which allows the simultaneous<br />

measurement of many (hkl) reflections (see Fig . 18 .14) and, finis, the collection of<br />

experimental data for many pole figures in only one sample scan . The pole figures are<br />

constructed (1) by conversion of the individual sample orientations (cp, x) into pole figure<br />

coordinates (a, ß), (2) by interpolation for points of an almost equispaced (a, ß)-grid in the<br />

pole figure projection (sec Fig . 18 .13) and (3) by graphically representing the pole figures<br />

with the corresponding reflection intensifies (compare Fig . 18 .15) .<br />

Fig . 18.15 : Comparison of c-axis polefigures (0001) ofa texturized quartzite obtainedfrom<br />

single grain analysis by U-stage inicroscopy (left) and neutron diffraction (right) based on<br />

investigations ofabout one hundred and one million grains, respectively .<br />

4.3 Pole Figures from <strong>Neutron</strong>s and X-Rays<br />

The advantages and drawbacks of both neutron and X-ray diffraction for texture analysis are<br />

obvions . Texture is a statistical description of ciystallite orientations and therefore requires a<br />

large number of ciystallites or grains in order to get a meaningful sampling . Reproducible<br />

18- 9

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