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Neutron Scattering

Neutron Scattering - JuSER - Forschungszentrum Jülich

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constant offset to the TOF . To be able to correct the TOF-histograms with respect to<br />

the spectral distribution of the incoming pulse, it is important to detected the incoming<br />

neutron flux by a monitor (Mo) located close to the sample position accumulated in a<br />

separate TOF-histogram . This type of TOF-spectrometer is preferentially used at pulsed<br />

sources, ideally it may be possible to omit the first chopper by taking the pulse as generated<br />

by the pulsed source (spallation target) . e All neutrons from the pulse (flying<br />

into the right direction) are utilized . This method has a few specific advantages and<br />

disadvantages, advantages are :<br />

1 . The pulse contains neutrons with high incident energy that may perform energy<br />

loss scattering, the resolution at high energy loss is relatively good, especially if the<br />

pulsed source supplies very short pulses ai high neutron energies .<br />

2 . If the analyzers are used in near backscattering configuration high resolutions (comparable<br />

to those on truc backscattering spectrometers, See chapter 9) can be attained<br />

.<br />

The utilization of the full spectrum has however also disadvantages :<br />

1 . The full "white" pulse enters the shielded sample detector spacc . Any parasitic<br />

scattering and any imperfection of the analyzing filters or failurc to absorb neutrons<br />

of "unused" final wavelength or direction leads to ilicreased background . In addition<br />

the background depends on the sample which makes correcting subtractions difficult .<br />

2 . Samples are hit by a higher integral flux and therfore become more radioactive .<br />

In general also "normal" TOF instruments perform better on a pulsed source in comparison<br />

with a reactor (if the average fluxes are equal) silice by synchronizing source and<br />

chopper only a small part of the generated neutrons (with the desired wavelength) are net<br />

used . The distance source-chopper may serve at the saine time as TOF-monochromator .<br />

In total the efficiency is comparable with the inverted type because in both cases on<br />

one ride of the sample the spectrum is restricted by filters/monochromators and on the<br />

other side the full spectrum is utilized and sorted according to the TOF . Energy transfer<br />

analysis without filter on any ride is impossible .<br />

'Te suppress background or to prevent "frame overlap" it may be nevertheless advisable to use an<br />

additional chopper .<br />

10- 19

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