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Neutron Scattering

Neutron Scattering - JuSER - Forschungszentrum Jülich

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I (Q, t) and the exact symmetry point location . This also holds if any perturbation shifts<br />

the location as indicated by the three hollow circles in the figure .<br />

P 1-__________<br />

I(Q,t)<br />

j1--1-<br />

I(Q,0)<br />

Symmetry<br />

Figure 11 .5 : Schematic echo form, idealized .<br />

For an ideal spectrometer I(Q,t)II(Q,0) = S(Q,t)IS(Q) would be the desired value of<br />

the normalized intermediate scattering function . In reality resolution effects and polarization<br />

losses reduce the value of I(Q, t)/I(Q, 0) compared to S(Q, t)/S(Q) .<br />

Figure 11 .6 shows data from actual experiments that are used to determine the echo<br />

amplitude and average intensity . Here the shape of the echo signal (intensity vs . symmetry<br />

current) is sampled for a considerably larger number than the minimum of three points .<br />

The parameters amplitude, average and phase zero current are determined by a nonlinear<br />

fit . Behind the oscillating echo form there are two further groups of points showing the<br />

minimum and maximum of intensity which indicates the efficiency of the polarization<br />

analysis . These intensities are measured by deactivating the 7r/2-flippers (minimum) and

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