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Geant4 Simulations for the Radon Electric Dipole Moment Search at

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30<br />

Absolute Efficiency (%)<br />

25<br />

20<br />

15<br />

10<br />

RnEDM Components<br />

no cell, oven or magnet<br />

cell and oven only<br />

magnet only<br />

cell, oven and magnet<br />

5<br />

0<br />

10 100 1000 10000<br />

γ-ray Energy (keV)<br />

Figure 4.2: <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 various<br />

components of <strong>the</strong> RnEDM appar<strong>at</strong>us.<br />

4.1.2 223 Rn β-Decay Spectra<br />

The β decay of 223 Rn into 223 Fr was simul<strong>at</strong>ed to include all known β decay<br />

branches and subsequent γ-ray, conversion electron and X-ray decays. The full γ-<br />

ray spectrum <strong>for</strong> <strong>the</strong> β decay of 223 Rn is presented in Figure 4.4(a). The <strong>Geant4</strong><br />

simul<strong>at</strong>ion consisted of 1.2 billion β decay events from an initial sample of 8 ×10 10<br />

nucleiinside<strong>the</strong>EDMcell. TheEDMcell, oven, magnetand1mmofµMetalshielding<br />

were included in <strong>the</strong> simul<strong>at</strong>ion. The initial polariz<strong>at</strong>ion was assumed to be 100% and<br />

both<strong>the</strong>spin-relax<strong>at</strong>ion(T 1 )and<strong>the</strong>spin-decoherence(T 2 )timesweresimul<strong>at</strong>edtobe<br />

30 seconds, resulting in a combined depolariz<strong>at</strong>ion time of 15 seconds. The simul<strong>at</strong>ed<br />

decay scheme (See Appendix A) includes 136 levels and 294 γ-ray transitions. The<br />

inclusion of <strong>the</strong> internal conversion process is shown to be important as <strong>the</strong> resulting<br />

X-rays domin<strong>at</strong>e <strong>the</strong> spectrum <strong>at</strong> low energies.<br />

63

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