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Neutron Scattering

Neutron Scattering - JuSER - Forschungszentrum Jülich

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if an increase in resolution may be achieved by stricter wavevector 1 selection (velocity,<br />

direction) and by reduction of the chopper pulse length, it is offen not advisable to<br />

enhance all elements of the resolution up to the technological limits because this goes along<br />

with a drastic loss of intensity (detector count rate) . Design of (neutron)-spectremet ers<br />

means the search for the Best compromise between resolution and intensity .<br />

The optimum<br />

depends on the nature of the problem, i .e . the features and structures expected in S(Q, 4 .<br />

TOF spectrometers as described in this chapter are preferentially used to investigate<br />

isotropie to weakly anisotropie samples with only weak structures in S(Q) . This enables<br />

the utilization of a large solid angle for detectinn which compensates for the loses caused<br />

by energy analysis . In the schematics of the spectrometers this is already indicated by<br />

the large number of detectors . Modern TOF instruments contain more than 1000 single<br />

counting tubes covering a detecting area of 30 x lcm 2 each . The total area coverd by<br />

1000 detectors is about 3m2 , for a flight path of 3 m this corresponds to a solid angle<br />

of 0.333 or 1000 degrees squared . Thereby an intesity gain of a factor 500 is obtained<br />

compared to a triple axis spectrometer with a detecting area of 2 degrees squared, the<br />

loss caused by the fact that the chopper opens only for about 1% of the time is more<br />

than compensated . In addition the TOF instrument has a multiple advantage : all energy<br />

transfers are detected simultaneously and not sequentially as in the case of a triple-axis<br />

spectrometer . However it is seldom useful to surr the data of ALL detectors into one<br />

spectrum but different scattering angle regions have to be evaluated separately. Still<br />

they are measured all at the saine time! Generally the TOF instrument is more efficient<br />

than a triple-axis spectrometer for isotropie samples . As soon as single crystals or very<br />

anisotropie samples with a strong dependence of the spectra on Q are to be investigated<br />

the conventional triple-axis spectrometers are better suited .

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