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Geant4 Simulations for the Radon Electric Dipole Moment Search at

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(a) Form<strong>at</strong>ion and<br />

breakup of an alkalimetal/noble-gas<br />

van<br />

der Waals molecule<br />

(b) Binary collision<br />

between an alkalimetal<br />

<strong>at</strong>om and a<br />

noble-gas <strong>at</strong>om<br />

Figure 2.5: Polariz<strong>at</strong>ion transfer process.<br />

negligible. For heavier noble gases, such as Xe and Rn, <strong>the</strong> contributions of van der<br />

Waals molecules domin<strong>at</strong>e over <strong>the</strong> contribution of binary collisions <strong>at</strong> low pressures.<br />

The pressure of <strong>the</strong> buffer gas particip<strong>at</strong>es in <strong>the</strong> cre<strong>at</strong>ion and destruction of <strong>the</strong><br />

<strong>for</strong>med alkai-metal noble-gas van der Waals molecule (Figure 2.5). At high pressures<br />

(multi<strong>at</strong>mosphere pressures) <strong>the</strong> collisions from N 2 gre<strong>at</strong>ly suppress <strong>the</strong> lifetime of<br />

<strong>the</strong> <strong>for</strong>med van der Waals molecule. Thus binary collisions domin<strong>at</strong>e <strong>the</strong> transfer of<br />

angular momentum.<br />

The RnEDM experiment will use high pressures in <strong>the</strong> measurement cell, where<br />

<strong>the</strong> N 2 gas also plays a role in <strong>the</strong> optical pumping process. The N 2 gas will nonradi<strong>at</strong>ively<br />

de-excite (“quenche”) <strong>the</strong> excited rubidium <strong>at</strong>oms be<strong>for</strong>e <strong>the</strong>y can reradi<strong>at</strong>e<br />

a photon. This avoids radi<strong>at</strong>ion trapping, where a photon is emitted by one<br />

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