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Geant4 Simulations for the Radon Electric Dipole Moment Search at

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a fully verified <strong>Geant4</strong> framework <strong>for</strong> <strong>the</strong> TIGRESS array [35]) was simul<strong>at</strong>ed to<br />

<strong>the</strong> highest degree of reality. The GUGI program was written to allow <strong>for</strong> a simple<br />

graphical manipul<strong>at</strong>ion of <strong>the</strong> input simul<strong>at</strong>ion parameters, allowing <strong>the</strong> user to<br />

quickly and effectively study many different aspects of <strong>the</strong> RnEDM simul<strong>at</strong>ion. The<br />

entire simul<strong>at</strong>ion package provides a powerful tool <strong>for</strong> fur<strong>the</strong>r studies of <strong>the</strong> RnEDM<br />

experiment <strong>at</strong> TRIUMF.<br />

The RnEDMexperiment will achieve anextremely sensitive measurement th<strong>at</strong> demands<br />

expertise in <strong>at</strong>omic and nuclear physics alongside advances in technology. The<br />

<strong>Geant4</strong> simul<strong>at</strong>ions <strong>for</strong> <strong>the</strong> RnEDM experiment valid<strong>at</strong>e <strong>the</strong> feasibility of measuring<br />

an <strong>at</strong>omic EDM using NMR techniques and γ-ray detection. The EDM measurement<br />

of 223 Rn would need a sensitivity on <strong>the</strong> order 1×10 −26 ecm [27], to be competitive<br />

with <strong>the</strong> current 199 Hg measurement of d( 199 Hg) ≤ 3.1×10 −29 ecm [19], while taking<br />

advantage of <strong>the</strong> predicted EDM enhancement factor of ∼ 600 <strong>for</strong> 223 Rn rel<strong>at</strong>ive to<br />

199 Hg [2]. The results presented in Chapter 4 show th<strong>at</strong> with 1 × 10 12 photopeak<br />

counts (equivalent to 100 days of counting [32]) detected in <strong>the</strong> GRIFFIN detectors,<br />

a sensitivity of 4.64×10 −26 ecm would be reached with an electric field of 5 kV/cm<br />

and a spin-decoherence time of 15 seconds. Increases in both E and/or T 2 through<br />

<strong>the</strong> EDM cell design will each improve <strong>the</strong> achievable sensitivity linearly.<br />

5.2 Future Directions<br />

The <strong>Geant4</strong> framework <strong>for</strong> <strong>the</strong> RnEDM experiment can be applied to many<br />

different applic<strong>at</strong>ions beyond <strong>the</strong> ones studied in this work. Firstly, <strong>the</strong> β decay<br />

package th<strong>at</strong> handles particle emission is a very general code. Any β process can be<br />

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