NeuLAND - FAIR
NeuLAND - FAIR
NeuLAND - FAIR
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clusters<br />
N<br />
100<br />
50<br />
0<br />
0 500 1000 1500<br />
total light (a.u.)<br />
Figure 4.16.: Same as in figure 4.15, but now for the data combined for all neutron<br />
multiplicities. The lines present the conditions which are applied in the<br />
further analysis to distinguish the different multiplicities.<br />
detected<br />
200 MeV<br />
generated<br />
% 1n 2n 3n 4n 5n<br />
1n 88 31 6 1 0<br />
2n 2 62 37 10 2<br />
3n 0 5 49 38 14<br />
4n 0 0 8 48 54<br />
5n 0 0 0 3 26<br />
6n 0 0 0 0 3<br />
detected<br />
600 MeV<br />
generated<br />
% 1n 2n 3n 4n 5n<br />
1n 92 22 2 0 0<br />
2n 2 71 32 7 1<br />
3n 0 6 55 32 9<br />
4n 0 0 10 57 50<br />
5n 0 1 1 4 35<br />
6n 0 0 0 0 5<br />
detected<br />
1000 MeV<br />
generated<br />
% 1n 2n 3n 4n 5n<br />
1n 89 12 1 0 0<br />
2n 7 78 23 3 0<br />
3n 0 8 63 26 5<br />
4n 0 0 12 63 40<br />
5n 0 0 0 7 46<br />
6n 0 0 0 0 8<br />
Table 4.5.: Neutron separation matrices for multiplicities of 1 to 5 neutrons. Columns<br />
display the neutron multiplicity simulated, rows the neutron multiplicity derived<br />
from the neutron tracking algorithm. Values are given in percent. Neutrons<br />
were simulated with 200 (left), 600 (middle) and 1000 MeV (right matrix).<br />
<strong>NeuLAND</strong> was located at a distance of 15.5 m to the target. Neutrons<br />
were generated with a relative energy of 500 keV with respect to a medium<br />
heavy projectile fragment. The distance between target and <strong>NeuLAND</strong> was<br />
filled with air.<br />
57