Diploma Thesis - Erich Schmid Institute
Diploma Thesis - Erich Schmid Institute
Diploma Thesis - Erich Schmid Institute
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X-ray Diffraction – Measurements and Alignment<br />
so that the centre of the top face is in the middle of the laser spot. Afterwards the<br />
shade holder together with the laser is removed and the detector is turned back to<br />
0° position. Afterwards a dial gauge is mounted in fro nt of the diffractometer plate to<br />
adjust the height to 5,75 mm.<br />
The top surface of the metallic block intersects with the ω−axis. If no radiation is<br />
detected by opened shutter the height of the monochromator is too low and all<br />
radiation will be adsorbed by the metallic block (figure 9.6a). Otherwise if it is too high<br />
the detector will measure the full intensity (figure 9.6b). To find the correct height the<br />
monochromator is moved in such a way that half of the maximum intensity is<br />
measured, so it is guaranteed that the X-ray beam intersects with the ω−axis<br />
(figure 9.6c).<br />
a.) Monochromator is too low b.) Monochromator is too high c.) X-ray beam intersects with<br />
rotation axe<br />
The fine adjustment is done by rotating the metal block around ω−axis. A scan shows<br />
that the intensity has a maximum at a certain ω−angle (figure 9.7). It is supposed that<br />
at the maximum intensity the top surface of the metallic block is parallel to the<br />
incident beam, so the deviation from the zero ω−angle can be electronically<br />
corrected. The last step is to measure gold standard like it is done in the point focus<br />
alignment.<br />
Figure 9.6: Height adjustment of the monochromator<br />
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