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Neutron Scattering

Neutron Scattering - JuSER - Forschungszentrum Jülich

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Fig . 18 .12 : Examples of crystallographic<br />

planes (top) and their<br />

accessory pole figures (bottom)<br />

for a two-dimensional (a) and a<br />

three-dimensional (b) single<br />

crystal with one fzxed pole per<br />

plane and for a polycrystalline<br />

sample (c and d) with a scatter of<br />

poles;<br />

(a) (001)plane and its counterpart<br />

(00-1) (north-south<br />

normal directions)<br />

(b) cubic Basis planes (100),<br />

(010), (001) (left) and Body<br />

diagonal planes {111} (right)<br />

(c)<br />

spread ofdierently oriented<br />

(001) planes<br />

(d) spread ofdierently oriented<br />

cubic Basis planes {1001<br />

4 .2 Experimental Pole figures<br />

An experimental (hkl) pole figure is obtained by diffraction methods by measuring the<br />

intensity of a Bragg reflection (hkl) for a variety of différent sample orientations . Usually, at<br />

least so far, one uses monochromatic neutrons (or X-rays) . The simplest instrumental setup is<br />

that of a four-circle diffractometer equipped with a Eulerian cradle (cp, x rotation axes) as<br />

sample goniometer (Fig . 18 .13) and a simple counting tube, i .e . an instrument as used for<br />

single crystal structure investigations . A stationaiy detector is positioned in thé peak<br />

maximum ofa reflection, and sample orientation dependent measurements are performed, e .g .<br />

in a step scanning mode, realizing an equal area pole figure grid (Fig . 18 .13) .<br />

Fig. 18 .13 : Eulerian cradle with rotation axes (p ,- (w = 20/2 position) (left) and typical<br />

(c5ß) - polefigure scanning grid (right)<br />

18- 8

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