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NeuLAND - FAIR

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8.1.2. Characterization of Neutron Interactions with the Full-Size<br />

Detector<br />

After the installation of the fully-equipped <strong>NeuLAND</strong>, again, a calibration experiment<br />

will be performed. The above-mentioned technique of quasi-free scattering of deuteron<br />

beams will be applied. Time resolution and efficiency of the full system will be determined,<br />

the latter as a function of neutron energy. Using the full detector volume, it<br />

allows in addition a detailed study of the event patterns for real one-neutron events.<br />

This is an important input for the development of tracking algorithms in order to optimize<br />

the recognition capabilities. The measured one-neutron response can be used in<br />

order to simulate the response of <strong>NeuLAND</strong> to multiple neutron events by overlaying<br />

several one-neutron hit-patterns, taken from experimental data. This method relies on<br />

the superposition principle for hit patterns on the <strong>NeuLAND</strong> detector.<br />

Moreover, <strong>NeuLAND</strong> will be exposed to real and clearly characterized two-neutron<br />

events, using the breakup of tritons as detailed in the following. Tritons provide a clean<br />

source of correlated two neutron events, where the intrinsic wave function is known with<br />

high precision. Quasifree proton knockout on the tritons with coincident detection of the<br />

two protons from the (p,2p) reaction enables us to put strict cuts on the reaction kinematics,<br />

in particular the transferred momentum to the removed proton. By requiring a<br />

momentum transfer considerable larger than the proton’s Fermi momentum inside the<br />

tritons we enhance events where the two neutrons act as spectators in the reaction, and<br />

thus keep their original correlations. Using the known n-n scattering length, also finalstate<br />

interaction can be taken into account precisely. The n-n relative-energy spectrum<br />

can thus be calculated reliably and compared to the observed spectrum. The response<br />

of the detector to 2n events is particularly important for low relative energy between the<br />

two neutrons, En−n, for which the efficiency drops rapidly. In addition, the incident CM<br />

angle of the two neutrons can be determined by the measurement of the angles of the<br />

two protons. This measurement will, thus, allow for a detailed check of the simulation<br />

procedure for the two neutron response.<br />

8.2. Cosmic Ray Tracking in <strong>NeuLAND</strong> for Adjustment and<br />

Calibration<br />

For the internal calibration of <strong>NeuLAND</strong> before, during and after experiments, tracks<br />

from cosmic rays will be used. The hard component of the cosmic ray flux at sea<br />

level, mainly muons (97%), has sufficiently high energy (mean energy is 2 GeV) to<br />

penetrate the concrete ceiling of the Cave C or the R 3 B Cave, respectively, and to<br />

traverse <strong>NeuLAND</strong> with approximately the speed of light. The expected rates of incident<br />

cosmic rays amount to about 1.5 kHz. That enables a full scan of the detector within<br />

reasonable time scales. The tracks of muons, as displayed in a GEANT4 simulation in<br />

figure 8.4, serve as a good time reference between the traversed submodules.<br />

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