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1 - IAEA Nuclear Data Services

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- 132 -<br />

.6. On 239 Pu<br />

A series of neutron scattering measurements on<br />

259<br />

^-\Pu<br />

were started at low primary neutron energies. For these<br />

experiments an especially developped "low threshold"<br />

neutron time-of-flight detector is in use. The detection<br />

threshold corresponds to a neutron energy of about<br />

40 keV. For the evaluation of the neutron scattering<br />

cross sections it is necessary to subtract from the<br />

measured spectra the contribution of the fission neutrons.<br />

The fission spectrum was measured with primary<br />

neutron energies around 60 keV. So far angular distributions<br />

of neutrons from<br />

259<br />

•'•'Pu have been measured at<br />

incoming energies of 0.4, 0.3 and 0.2 MeV.<br />

.7. Experimental Equipment<br />

A detecting system consisting of four counters for<br />

simultaneous detection of neutrons scattered at different<br />

angles was brought into operation. So far only<br />

three counters were used for measuring neutron angular<br />

distributions, while the fourth was used as a<br />

neutron time-of-flight monitor. The general lay-out<br />

of the experimental arrangement is shown in fig. 5.<br />

Ion Source Test Facility<br />

K.H. Bbckhoff, A. Crametz<br />

The first stage of the 150 keV accelerator was put<br />

in operation. Protons of about 1 mA have been accelerated<br />

to 30 keV and sharply focussed onto a graphite<br />

target.<br />

Linear Accelerator<br />

Total Gross Sections<br />

.1. Resonance Range<br />

K.H. Bôckhoff, V. Kolar<br />

?40<br />

The measurements and analysis of the neutron total

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