Geant4 Simulations for the Radon Electric Dipole Moment Search at

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[36] M. A. Schumaker and et al. Nucl. Instrum. Meth. A, 570:437–445, 2007. [37] S. Agostinelli et al. Nucl. Instr. and Meth. A, 506:250–303, 2003. [38] Geant4 collaboration, January 2011. http://geant4.web.cern.ch/geant4/collaboration/index.shtml. [39] pyrex glass specifications, January 2011. http://catalog2.corning.com/Lifesciences/media/pdf/Description of 7740 Glasses.pdf. [40] mu-metal specifications, January 2011. http://www.mumetal.com/mumetal specifications.html. [41] cerium-doped lanthanum bromide specifications, January 2011. http://www.oilandgas.saint-gobain.com/uploadedFiles /SGoilandgas/Documents/Detectors/Detectors-BrilLanCe-380.pdf. [42] Saint-Gobain Crystals. BrilLanCe tm scintillators performance summary. Technical report, Saint-Gobain Crystals, Scintillation Products, January 2009. [43] W. Kurcewicz and et al. Nucl. Phys. A, 539:451–477, 1992. [44] T. Kibédi, T.W. Burrows, M.B. Trzhaskovskaya, P.M. Davidson, and C.W. Nestor Jr. Nucl. Instr. and Meth. A, 589:202–229, 2008. [45] Philip Bevington and D. Keith Robinson. Data Reduction and Error Analysis for the Physical Sciences. McGraw-Hill, 2002. [46] Kai Siegbahn. Alpha-, beta- and gamma-ray spectroscopy. North-Holland Publishing Company, 1965. 106
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GEANT4 SIMULATIONS FOR THE RADON EL
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Dictated but not read. i
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Contents Acknowledgements ii 1 Intr
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4 Results 60 4.1 γ-Ray Spectroscop
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List of Figures 1.1 An illustration
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Chapter 1 Introduction Thesearchfor
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ˆP ր ˆT ց Figure 1.1: An illust
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1.1.1 CP Violation Following the ob
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Figure 1.2: Experimental upper limi
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Figure 1.3: Illustration of the dou
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Chapter 2 RnEDM Experiment at TRIUM
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Figure 2.1: A schematic of the ISAC
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a measurement cell. The RnEDM exper
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NMR techniques, and supplementing s
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Occupied Orbitals Fine Structure Hy
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energy levels are separated accordi
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(σ + ) along the axis of the B fie
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atom and absorbed by another. Radia
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anaverageof120kHzphotopeakcountrate
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Figure 2.7: One GRIFFIN/TIGRESS HPG
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(a) One GRIFFIN detector in the HPG
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3.1 Introduction 3.1.1 Previous Wor
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energies, branching ratios, emissio
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used around the measurement cell in
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3.2.5 Simulated Data Thecodewaswrit
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lower its total energy. Internal co
Page 53 and 54:
10000 1000 2 χ red = 1.21 t 1/2 =
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as [47] I(E) = G 2π 3 7 c 6 | M i
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was to use an average X-ray energy
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1.5 1.4 1.3 1.2 P = 100% P = 75% P
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where (a b c d | e f) are Clebsch-G
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2 2 1.5 J i = 5/2, J f = 5/2 J i =
Page 65 and 66: of radius 10 cm, allowing the GRIFF
Page 67 and 68: (a) Screenshot showing the detector
Page 69 and 70: 3.6.2 Output Data and Sort Codes Th
Page 71 and 72: (user-defined option), secondly toa
Page 73 and 74: 30 Absolute Efficiency (%) 25 20 15
Page 75 and 76: 11 10 9 8 7 6 5 4 3 2 1 0 1e+06 Cou
Page 77 and 78: 4.2.1 Multipolarity Effects The sha
Page 79 and 80: Figure 4.7: The time projections an
Page 81 and 82: distribution, this average intensit
Page 83 and 84: Table 4.1: The fit results for the
Page 85 and 86: 12 10 linear regression: y = 0.2243
Page 87 and 88: 15 Linear Counts (e+04) 10 5 0 1e+0
Page 89 and 90: Chapter 5 Conclusions and Future Di
Page 91 and 92: simulated given sufficient parent a
Page 93 and 94: Appendix A Figure A.1: Simulated de
Page 95 and 96: Figure A.3: Simulated decay scheme
Page 97 and 98: Figure A.5: Simulated decay scheme
Page 99 and 100: 6 out = (1/(1+∆ˆ2))*(f(k,jf,L1,L
Page 101 and 102: 44 return; 45 end 46 if abs(m) > j
Page 103 and 104: 1 % LegendreP.m 2 function P = Lege
Page 105 and 106: 39 xx(i+1,j+1) = r(i+1,1)*sin((i*re
Page 107 and 108: 11 %warning('m1 + m2 + m3 must equa
Page 109 and 110: 23 end 24 % ////////// 25 j1 = J1;
Page 111 and 112: 33 if L1 == L2 && ∆ == 0 34 title
Page 113 and 114: Bibliography [1] J. M. Pendlebury a
Page 115: [25] P. G. Bricault, M. Dombsky, Je
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