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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Absolute Efficiency (%)<br />
15<br />
10<br />
5<br />
µMetal Thickness<br />
0.10 cm<br />
0.25 cm<br />
0.50 cm<br />
0.75 cm<br />
1.00 cm<br />
0<br />
100 1000 10000<br />
γ-ray Energy (keV)<br />
Figure 4.3: <strong>Geant4</strong> gener<strong>at</strong>ed absolute efficiency curves <strong>for</strong> a ring of eight GRIFFIN<br />
detectors in <strong>the</strong> highest efficiency mode (<strong>for</strong>ward configur<strong>at</strong>ion) including <strong>the</strong> full<br />
RnEDM setup (EDM cell, oven and magnet) with various thicknesses of µMetal.<br />
Timing in<strong>for</strong>m<strong>at</strong>ion was extracted from γ-ray energy-time m<strong>at</strong>rices. Figure 4.4(b)<br />
illustr<strong>at</strong>es a three-dimensional view of a small energy and time slice <strong>for</strong> one detector<br />
in <strong>the</strong> simul<strong>at</strong>ion presented in Figure 4.4(a). The dimension of <strong>the</strong> γ-ray energy-time<br />
m<strong>at</strong>rices were 4096 by 4096, where <strong>the</strong> γ-ray energies were binned into 1 keV bins<br />
resulting in a maximum energy of about 4.1 MeV. The resolution of <strong>the</strong> time bins<br />
was flexible and thus optimized <strong>for</strong> <strong>the</strong> length of each simul<strong>at</strong>ion. Generally <strong>the</strong> times<br />
were binned into 10 ms, resulting in just over 40 seconds of simul<strong>at</strong>ion time.<br />
4.2 Frequency Signal<br />
The frequency signal can be clearly seen in <strong>the</strong> three-dimensional Figure 4.4(b).<br />
To gener<strong>at</strong>e a spectrum of this signal, energy g<strong>at</strong>es were placed around <strong>the</strong> γ-ray<br />
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