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Neutron Scattering

Neutron Scattering - JuSER - Forschungszentrum Jülich

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select a special wavelengths band (;, ± Ak/;,) out of the "white" beam according to the Bragg<br />

condition for its scattering plane (hkl)<br />

2dhk1' SinO yk1 = ;~ ,<br />

with the interplanar spacing dhkl and the monochromator scattering angle 26hk1 = 20m. The<br />

width ofthe wavelengths band which is important for the Q-resolution, depends on the<br />

divergences of the beam before and after the monochromator (collimations al and a2), on the<br />

mosaic spread of the monochromator crystal AM, and on the monochromator angle 20m. In<br />

order to increase the intensity of the monochiomatoc beam at the sample position the<br />

monochromator cystal is often bent in vertical direction perpendicular to the diffraction plane<br />

of the experiment. In this way the vertical beam divergence is increased leading to a loss of<br />

resolution in the reciprocal space . Thc diffracted intensity from the sample is measured as a<br />

function of the scattering angle 26 and the sample orientation (especially in case of a single<br />

cystal) :<br />

for a single crystal ---> I(Q), and for a polycrystalline sample -> I( I Q 1 ) .<br />

29 is defmed by the collimators a2 and a 3 . As there is no analysis of the energy of the<br />

Detector<br />

Fig . 1 . Schematic representation of a 2-axes diffractometer .<br />

7-2

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