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NeuLAND - FAIR

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events<br />

800<br />

600<br />

400<br />

200<br />

0<br />

0 200 400 600 800 1000<br />

total light (a.u.)<br />

events<br />

600<br />

400<br />

200<br />

0<br />

0 50 100 150<br />

multiplicity<br />

Figure 4.14.: Left hand side: Total energy deposited in <strong>NeuLAND</strong> from 600 MeV neutrons<br />

for multiplicities of 1 (black), 2 (green), 3 (red), 4 (blue), 5 (yellow)<br />

and 6 (magenta). Right hand side: Multiplicity from number of submodules<br />

with valid signals, again for 1 to 6 neutrons impinging with 600 MeV.<br />

4.5.3. Neutron Tracking<br />

For the final assignment of neutrons we now utilize the calorimetric information for<br />

the neutron multiplicity. Typically, the number of clusters in the event is much larger<br />

than the derived neutron multiplicity, as detailed before. We, therefore, have to select<br />

from the list of clusters the ones that are most reliable, thus ensuring that also the<br />

correct momenta of neutrons are reconstructed. The time-wise first cluster is taken as<br />

the first neutron track. For the remaining clusters, a resorting procedure is performed.<br />

An excellent criterion appears to be a combined requirement on the smallest difference<br />

of velocity of the neutron βcluster (associated with the cluster), the beam velocity βbeam<br />

and the largest energy deposit of the cluster Ecluster dep . The clusters are sorted according<br />

to their values of<br />

Rcluster = |βcluster − βbeam|<br />

E cluster<br />

dep<br />

(4.2)<br />

starting with the smallest value of Rcluster. Finally, clusters from this sorting are defined<br />

as neutron tracks up to the maximum number of neutrons from the calorimetry<br />

argument. The remaining clusters are eliminated from the further analysis.<br />

The quality of the neutron detection and its separation into the various multiplicities can<br />

be understood from the so-called neutron separation matrices, displayed in tables 4.5 for<br />

200, 600 and 1000 MeV neutrons impinging on <strong>NeuLAND</strong>, at a distance of 15.5 m to<br />

the origin of the neutrons. For multiplicities of up to 5 neutrons simulated (columns),<br />

the percentage of detection in the various neutron channels derived from the tracking<br />

algorithms is indicated, respectively (rows).<br />

55

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