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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simul<strong>at</strong>ed given sufficient parent and daughter nucleus in<strong>for</strong>m<strong>at</strong>ion. A n<strong>at</strong>ural extension<br />
to <strong>the</strong> simul<strong>at</strong>ion would be <strong>the</strong> option of including of radioactive contamin<strong>at</strong>ion.<br />
The first tests with <strong>the</strong> ISAC uranium-carbide target in December 2010 indic<strong>at</strong>ed<br />
an overwhelming presence of francium. Alkali metals, such as francium, are readily<br />
ionized through surface ioniz<strong>at</strong>ion. It is very likely th<strong>at</strong> <strong>the</strong> RnEDM experiment will<br />
have some contamin<strong>at</strong>ion from francium. Including radioactive contamin<strong>at</strong>es into<br />
<strong>the</strong> <strong>Geant4</strong> simul<strong>at</strong>ion could help study <strong>the</strong> contamin<strong>at</strong>ion effect on <strong>the</strong> observed<br />
precession frequencies, and thus <strong>the</strong> EDM sensitivity.<br />
The final design <strong>for</strong> <strong>the</strong> RnEDM measurement remains under development. The<br />
<strong>Geant4</strong> simul<strong>at</strong>ions can be used to study <strong>the</strong> effect of γ-ray sc<strong>at</strong>tering and backgrounds<br />
in <strong>the</strong> experimental appar<strong>at</strong>us <strong>for</strong> various m<strong>at</strong>erials and geometries. The<br />
optimiz<strong>at</strong>ion of <strong>the</strong> m<strong>at</strong>erials and geometries of <strong>the</strong> RnEDM appar<strong>at</strong>us can lead to<br />
improved detection efficiencies.<br />
Finally, <strong>the</strong> simul<strong>at</strong>ion of Saint-Gobain’s BrilLanCe 380 LaBr 3 (Ce) detector can<br />
be improved by modeling <strong>the</strong> true aluminum construction around <strong>the</strong> crystal and<br />
including <strong>the</strong> radioactive n<strong>at</strong>ure of 138 La. 138 La is a n<strong>at</strong>urally occurring radioisotope<br />
(0.09% abundance [41]) with a long half-life of 1.05×10 11 years[49]. It decays with<br />
a 66.4% probability of electron capture into an excited st<strong>at</strong>e in 138 Ba, which in turn<br />
decays by <strong>the</strong> emission of a 1426keV γ ray. The remaining 33.6%decays via β − decay<br />
into an excited st<strong>at</strong>e in 138 Ce, which in turn decays by <strong>the</strong> emission of a 789 keV γ<br />
ray in coincidence with <strong>the</strong> emitted electron [49]. There<strong>for</strong>e <strong>the</strong> LaBr 3 (Ce) detectors<br />
contain internal radi<strong>at</strong>ion peaks which can be incorpor<strong>at</strong>ed into <strong>the</strong> <strong>Geant4</strong><br />
simul<strong>at</strong>ions <strong>for</strong> added realism.<br />
The search <strong>for</strong> particle and <strong>at</strong>omic EDMs is an important area of physics research<br />
today, as it directly probes <strong>the</strong> fundamental symmetries of <strong>the</strong> laws of physics.<br />
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