Geant4 Simulations for the Radon Electric Dipole Moment Search at
Geant4 Simulations for the Radon Electric Dipole Moment Search at
Geant4 Simulations for the Radon Electric Dipole Moment Search at
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200<br />
2<br />
χ red<br />
= 1.001<br />
f = 2.0010(2) Hz<br />
Counts<br />
3400<br />
3200<br />
3000<br />
2800<br />
2600<br />
0 5 10 15 20 25 30<br />
Seconds (500ms Time Bins)<br />
Counts<br />
150<br />
100<br />
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15<br />
Seconds (20ms Time Bins)<br />
Figure 4.14: The fit of <strong>the</strong> 565 keV to 614 keV energy g<strong>at</strong>e time projection <strong>for</strong> two<br />
anti-parallel BrilLanCe 380 LaBr 3 (Ce) detectors.<br />
Figure 4.4(a). The figure shows th<strong>at</strong> not all individual photopeaks are resolved with<br />
<strong>the</strong> LaBr 3 (Ce) detectors. Figure 4.14 illustr<strong>at</strong>es <strong>the</strong> time projection and fit of a g<strong>at</strong>e<br />
set between 565 and 614 keV. Although <strong>the</strong> g<strong>at</strong>e encompasses many photopeaks <strong>the</strong><br />
frequency signal is still clearly visible and fur<strong>the</strong>r explor<strong>at</strong>ion of <strong>the</strong> use of <strong>the</strong> highr<strong>at</strong>e<br />
capabilities of LaBr 3 (Ce) scintill<strong>at</strong>ors in <strong>the</strong> RnEDM experiment is warranted.<br />
78