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Neutron Scattering

Neutron Scattering - JuSER - Forschungszentrum Jülich

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18 . Texture in Materials and Earth Sciences<br />

Wolfgang Schäfer<br />

Mineralogisch-Petrologisches Institut, University ofBonn<br />

Forschungszentrum Jülich, MIN/ZFR, 52425 Jülich<br />

1.0 Introduction<br />

The topic texture` has to be assigned to the contributions about elastic neutron scattering and<br />

the determination of crystal and magnetic structures by means ofBragg scattering using either<br />

polyciystalline or single crystalline samples (compare Fig .18 .la and 18 .1d, resp .) . When<br />

performing powder diffraction for the puiposes of refmements or even determinations of<br />

crystal (or magnetic) structures, one initially assumes statistical distributions of all crystallite<br />

orientations inside the polycrystalline material, thus ensuring that for the measurement ofeach<br />

Bragg reflection hkl an almost equal and, with respect to statistical relevance, a sufficient<br />

number of crystallites (small single crystals) is in reflection position . This is the prerequisite<br />

for an even intensity distribution on the Debye-Scheuer cones of a powder measurement (see<br />

Fig . 18 .1a) . Non-statistical distributions of crystallites, e .g. in case of plate- or rod-like cystal<br />

grains or for non-powderized bulk sample material, result in prefeued orientations of special<br />

scattering planes hkl and cause uneven (orientation dependent) intensity distributions on the<br />

Debye-Scherrer cones (sec Fig . 18 .lb and 18 .1c) appraoching the appearance of single crystal<br />

spots (Fig . 18 .1d) . The evolution of experimental intensities in crystal structure analysis is<br />

generally hampered by the presence of preferred orientation . For instance, special correction<br />

terms have to be applied during structure refmement calculations .<br />

(a) (b) (c) (d)<br />

Fig. 18.1 : hkl diffraction maxima (here X-ray scattering) shown as sectionsfrom Debye-<br />

Scherrer cones obtainedfrom polycrystalline material ofrandom crystallite orientations (a),<br />

weak (b) and strong (c) prefeued orientations. (d) shows single crystal diffraction spots.<br />

18-1

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