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Geant4 Simulations for the Radon Electric Dipole Moment Search at

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1.5<br />

1.4<br />

1.3<br />

1.2<br />

P = 100%<br />

P = 75%<br />

P = 50%<br />

P = 25%<br />

P = 0%<br />

1.1<br />

W(θ)<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0 π π 3π π 5π 3π 7π 2π<br />

4 2 4 4 2 4<br />

θ<br />

Figure 3.3: β particle angular distributions <strong>for</strong> various degrees of polariz<strong>at</strong>ion. The<br />

beta-asymmetry correl<strong>at</strong>ion coefficient was simul<strong>at</strong>ed to be 0.45.<br />

As <strong>the</strong> degree of polariz<strong>at</strong>ion reduces from its maximum value of 100% to 0% <strong>the</strong><br />

angular distribution of <strong>the</strong> electrons becomes more isotropic as shown in Figure 3.3.<br />

3.4.2 Gamma-Ray Anisotropies<br />

The <strong>the</strong>ory of angular distributions of γ radi<strong>at</strong>ion from oriented nuclei is well<br />

established [51, 52, 53]. The work from H.A. Tolhoek and J.A.M. Cox [51] derives<br />

<strong>for</strong>mula <strong>for</strong> oriented nuclear spins assuming pure multipole transitions. For a more<br />

general approach, T. Yamazaki [52] has outlined <strong>the</strong> general <strong>the</strong>ory and tabul<strong>at</strong>ed<br />

coefficients <strong>for</strong> γ-ray angular distributions <strong>for</strong> aligned and partially-aligned nuclei<br />

<strong>for</strong> pure and mixed multipolarities. Alignment, polariz<strong>at</strong>ion and orient<strong>at</strong>ion can have<br />

variousdefinitions. Inthis workand <strong>the</strong>work ofYamazaki <strong>the</strong>y aredefined asfollows.<br />

Alignment refers to symmetric popul<strong>at</strong>ions of magnetic subst<strong>at</strong>es about m = 0, thus<br />

49

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