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Neutron Scattering - JUWEL - Forschungszentrum Jülich

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16 POWDER DIFFRACTOMETER SPODI<br />

The flux from neutron sources much lower compared to X-ray tubes or even synchrotrons. In<br />

addition, neutrons interact weakly with matter. Therefore, much larger sample amounts are<br />

required compared to X-ray diffraction (“grams instead of milligrams”). On the other hand<br />

this weak interaction results in much higher penetration depths of neutrons, compared to<br />

laboratory X-ray diffractometers. Thus, polycrystalline bulk samples can be investigated.<br />

Furthermore, using large sample volumes avoids possible problems due to preferred<br />

orientation effects. In principle, bulk samples can also be investigated with high-energy<br />

synchrotron radiation. Anyhow in special cases the very low scattering angles related to low<br />

wavelength (in high-energy synchrotron studies) can cause difficulties.<br />

Sample environments<br />

The large penetration depths of neutrons facilitate the usage of sample environments like<br />

cryostat, furnaces, magnets... In general neutron scattering experiments are more powerful<br />

applying high or low temperatures. On the other hand, the small sample volume required for<br />

synchrotron studies gives better possibilities for high-pressure experiments.<br />

III) neutrons exhibit a magnetic moment<br />

Though neutrons do not have an electric charge, the internal charge distribution due to its<br />

three quarks along with the spin result in a magnetic moment of the neutron.<br />

implications:<br />

magnetic scattering<br />

The interaction between the magnetic moment of the neutron and a possible magnetic<br />

moment of an atom results in a magnetic scattering contribution, incidentally in the same<br />

order of magnitude as the nuclear scattering contribution. The magnetic scattering<br />

contribution can be easily detected by means of neutron diffraction. In synchrotron diffraction<br />

studies, possible magnetic scattering events are by several orders of magnitude weaker than<br />

the Thomson scattering.

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