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Geant4 Simulations for the Radon Electric Dipole Moment Search at

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Figure 2.7: One GRIFFIN/TIGRESS HPGe clover comprised of four individual crystals.<br />

Each crystal is 90 mm in length and 60 mm in diameter and has an efficiency<br />

of 40% rel<strong>at</strong>ive to a standard 3”× 3” NaI(Tl) crystal <strong>for</strong> 662 keV γ rays.<br />

14.5 cm. The front suppressors in this configur<strong>at</strong>ion also have <strong>the</strong> option of being<br />

collim<strong>at</strong>ed with a dense metal (hevimet). The dense metal, composed mostly of<br />

tungsten, prevents γ rays from directly hitting <strong>the</strong> front suppression shields.<br />

The GRIFFIN spectrometer is very similar in external geometry to its sister array<br />

TIGRESS (TRIUMF-ISAC Gamma-Ray Escape Suppressed Spectrometer) [33],<br />

which currently resides in <strong>the</strong> ISAC-II experimental hall <strong>at</strong> TRIUMF. The primary<br />

difference between <strong>the</strong> two designs is th<strong>at</strong> a TIGRESS detector has each HPGe crystal<br />

electrically segmented into 8 segments. This results in 32 electrical signals (plus<br />

four addition core contacts) per clover, whereas a GRIFFIN detector will have only<br />

4 electrical signals (<strong>the</strong> four core contacts) per clover. The principle reason <strong>for</strong> TI-<br />

GRESS’s highly segmented crystals is to provide three-dimensional localiz<strong>at</strong>ion of<br />

γ-ray interactions inside <strong>the</strong> crystals [34], which is necessary <strong>for</strong> experiments with<br />

<strong>the</strong> acceler<strong>at</strong>ed radioactive ion beams <strong>at</strong> ISAC-II. GRIFFIN, on <strong>the</strong> o<strong>the</strong>r hand, will<br />

reside in <strong>the</strong> ISAC-I hall and will be used primary as a decay spectrometer with<br />

low-energy radioactive ion beams. The segment<strong>at</strong>ion of <strong>the</strong> TIGRESS detectors is<br />

29

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