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Electron Neutrino Appearance in the NOνA Experiment Ji Liu Hainan, China Master of Science ... PDF

218 Pages·2016·22.93 MB·English
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FERMILAB-THESIS-2017-01 Electron Neutrino Appearance in the NOνA Experiment Ji Liu Hainan, China Master of Science, College of William and Mary, 2010 Bachelor of Physics, University of Science and Technology of China, 2009 A Dissertation presented to the Graduate Faculty of the College of William and Mary in Candidacy for the Degree of Doctor of Philosophy Department of Physics The College of William and Mary January 2017 Operated by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the United States Department of Energy (cid:13)c 2017 Ji Liu All rights reserved. APPROVAL PAGE This Dissertation is submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy Ji Liu Approved by the Committee, November, 2016 Committee Chair Associate Professor Patricia Vahle, Physics The College of William and Mary Professor Jeff Nelson, Physics The College of William and Mary Professor Todd Averett, Physics The College of William and Mary Assistant Professor Justin Stevens, Physics The College of William and Mary Associate Professor Robert Craig Group, Physics University of Virginia ABSTRACT The NuMI Off-Axis ν Appearance (NOνA) experiment is a long baseline, off-axis e neutrino oscillation experiment. It is designed to search for oscillations of ν to ν by µ e comparing measurements of the NuMI beam composition in two detectors. These two detectors are functionally identical, nearly fully-active liquid-scintillator tracking calorimeters and located at two points along the beam line to observe the neutrinos. The Near Detector (ND), situated 1km away from the proton target at Fermilab, measures neutrinos prior to oscillation. Then the Far Detector (FD), located 810 km away at Ash River, Minnesota, measures the neutrinos after they have traveled and potentially oscillated. The neutrino beam is generated at Fermi National Accelerator Laboratory in Batavia, Illinois by the Neutrinos at the Main Injector (NuMI) facility. By observing the ν → ν oscillation, NOνA is capable of measuring the neutrino mass µ e hierarchy, CP violation and the octant of mixing angle θ . This thesis presents the first 23 measurement of ν appearance in the NOνA detectors with 3.52×1020 protons-on-target e (POT) data accumulated from February 2014 till May 2015. In this analysis the primary ν CC particle selection LID observes 6 ν like events in the far detector with a e e background prediction of 0.99±0.11 (syst.), which corresponds to a 3.3σ excess over the no-oscillation hypothesis. This results disfavors 0.1π < δ < 0.5π in the inverted mass cp hierarchy at 90% C.L with the reactor constrain on θ . 13 TABLE OF CONTENTS Acknowledgments vi Dedication vii List of Tables viii List of Figures xi CHAPTER 1 The Physics of Neutrinos 1 1.1 A Brief Experimental History of Neutrinos 1 1.1.1 Discovery of Neutrinos 1 1.1.2 Neutrino Oscillation 4 1.2 Neutrinos in the Standard Model 7 1.2.1 Basic Ingredients of the Standard Model 7 1.2.2 Weak Force and Interactions 11 1.2.3 Neutrino Mass in the Standard Model 14 1.3 Neutrino Oscillations 16 1.3.1 Three-Flavor Neutrino Oscillations 19 1.3.2 Two-Flavor Neutrino Oscillations 23 1.3.3 Neutrino Oscillations in Matter 24 i 1.4 Neutrino Oscillations Experiments 27 1.4.1 Reactor Antineutrino Experiments 27 1.4.2 Accelerator Neutrino Experiments 29 1.5 Summary and Current Status 30 2 The NOνA Experiment 32 2.1 NOνA Overview and Physics goals 32 2.2 The NuMI Beamline 34 2.2.1 Basic Principle 35 2.2.2 The Target 36 2.2.3 Electromagnetic Focusing Horns 39 2.2.4 Decay Volume and Absorber 40 2.2.5 NuMI Upgrade 41 2.3 Off-Axis Features 42 3 The NOνA Detector 45 3.1 The NOνA Detector Design 45 3.1.1 The Basic NOνA Detector Element 47 3.1.2 Liquid Scintillator 48 3.1.3 Wavelength-Shifting Fiber 49 3.1.4 Photodetector and Electronics 49 3.1.5 PVC Modules 54 3.2 Assembly of NOνA Detectors 57 ii 4 Monte Carlo Simulation 63 4.1 NOνA Simulation Chain 63 4.2 Neutrino Interaction Physics Models in GENIE 65 4.2.1 Cross Section Model 66 4.2.2 Neutrino-induced Hadron Production 68 4.2.3 Intranuclear Hadron Transport 68 4.2.4 Nuclear Physics Model 70 5 Calibration and Event Reconstruction 71 5.1 Calibration 71 5.1.1 Attenuation Calibration 73 5.1.2 Absolute Energy Calibration 75 5.1.3 Timing Calibration 77 5.2 Reconstruction 77 5.2.1 Slicer4D 78 5.2.2 Hough Transform 81 5.2.3 Elastic Arm Vertex Finding 84 5.2.4 Fuzzy K-Means Algorithm 86 6 ν Event Selection 89 e 6.1 NOνA Event Topologies 90 6.2 Data Quality Selection 90 6.2.1 Beam Quality 91 iii 6.2.2 Subrun Data Quality 92 6.3 ν Event Selection 94 e 6.3.1 Reconstruction Quality Cuts 95 6.3.2 Containment Cuts 96 6.3.3 Cosmic Ray Rejection for Far Detector 99 6.3.4 Preselection Cuts 100 6.4 ν Particle Identification 102 e 7 ν Appearance Analysis 106 e 7.1 First Measurement Data 106 7.2 Data vs. MC Comparisons 108 7.2.1 ND Data vs. MC Comparison 109 7.2.2 FD Data vs. MC Comparison 114 7.3 Decomposition 117 7.4 Extrapolation 118 7.5 Far Detector Background and Signal Prediction 122 8 Systematics 126 8.1 Beam Systematic Uncertainties 127 8.2 Scintillator Saturartion Systematic Uncertainties 130 8.3 Calibration Systematic Uncertainties 131 8.4 Light Level Systematic Uncertainties 135 8.5 Neutrino Interaction Systematic Uncertainties 137 iv 8.6 Containment 152 8.7 Rock Contamination 153 8.8 Decomposition 154 8.9 Alignment 155 8.10 Data and Monte Carlo Statistics 156 8.11 Normalization 157 8.12 Summary 157 9 Results 159 9.1 Sideband Study 159 9.2 NOνA ν Appearance Result 160 e 9.2.1 ν Appearance Candidates 161 e 9.2.2 Confidence Interval 171 9.3 Conclusion 178 BIBLIOGRAPHY 179 v ACKNOWLEDGMENTS First and foremost I want to thank my advisor Patricia Vahle. For your guidance and mentorship through the whole journey of my Ph.D. For your enthusiasm and knowledge to neutrino physics that benefited a lot to both my study and this thesis. For your patient and support during the past 7 years when I tried to balance my research and personal life. I’m truly grateful to have you as my Ph.D advisor. I want to thank Professor Jeff Nelson, who introduced me to the Neutrino group of William and Mary and has been one of my committee for every annual review. Thank you for all your suggestions and ideas through all these years. I want to thank the other members of my graduate committee: Todd Averett, Robert Craig Group and Justin Stevens, for your time and effort to review my thesis and give valuable suggestions. I want to thank all the members in the NOνA collaboration, who has been doing an excellent job in putting together the detectors and collecting data. Especially I want to thank the ν appearance analysis group, this thesis would not be possible without the e contribution from each group member. The group conveners Patricia Vahle and Mayly Sanchez, thank you for your guidance and valuable suggestions. All the members in the ν group, including but not limit to: Alex Radovic, Chris Backhouse, Evan Niner, Tian e Xin, Kanika Sachdev, Hongyue Duyang, Jianming Bian, Erika Catano-Mur, and Xuebing Bu, thank you for all the discussion and help during this analysis. I also would like to thank all the members in the Neutrino group of William and Mary: Patricia Vahle, Jeff Nelson, Mike Kordosky, Alex Radovic, Alena Devan, Anne Norrick, Marco Colo, Dun Zhang and Leonidas Aliaga-Soplin. Thank you for all the good time that we work and travel together. Above all, I would like to extend a heartfelt thanks to my family. Thank you, mom and dad, for raising me up with all your love and supporting all my decisions. Lastly, thank you, my dearest husband Siyuan, for your love and encouragement, for always being there for me every step through this journey. vi

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A Dissertation presented to the Graduate Faculty .. 5.6 2D distribution of completeness vs. purity of the Slicer4D algorithm. For 5.7 The first iteration of the Hough transform shows in the event display (left) .. experiment in Ontario, Canada finally solved the solar neutrino problem and provided
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