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Beyond The Standard Model Explanations To Flavor Observables : 맛깔 관측량에 대한 표준 모형 너머의 설명

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dc.contributor.advisor김형도-
dc.contributor.author모도영-
dc.date.accessioned2017-07-19T06:09:15Z-
dc.date.available2017-07-19T06:09:15Z-
dc.date.issued2015-08-
dc.identifier.other000000067464-
dc.identifier.urihttp://dcollection.snu.ac.kr:80/jsp/common/DcLoOrgPer.jsp?sItemId=000000067464-
dc.description학위논문(박사)--서울대학교 대학원 :자연과학대학 물리·천문학부,2015. 8. 김형도.-
dc.description.abstractAfter 125 GeV Higgs boson discovery, minimal supersymmetric standard model with gauge mediation becomes dangerous. Gauge mediation is thought to be one of the simplest solutions for SUSY flavor problem, such a virtue of gauge mediation is now in danger. In this thesis, we consider right-handed Majorana neutrino as supersymmetry breaking messenger. We can get additional tri-linear
coupling AU at the messenger scale after integrating out the right-handed Majorana neutrino. Through additional AU term, we can realize maximal stop mixing scenario which is hardly possible in genuine gauge mediation mechanism. However, mediating SUSY breaking effects through Yukawa coupling reintroduces the SUSY flavor problem in the model unless neutrino Dirac Yukawa is proportional to identity matrix. Making neutrino Dirac Yukawa the identity matrix is not a bizzarre assumption, but it is easily achieved by importing discrete symmetry. Discrete symmetry is also useful to explain the tri-bi maximal form of the PMNS matrix. Tri-bi maximal form indicates the zero θ13 mixing of neutrinos, which is rejected by RENO and Daya Bay collaborations. To incorporate non-zero θ13, we introduce small deviation parameters in the Majorana mass matrix and neutrino Dirac Yukawa matrix. Deviation parameters in the neutrino Dirac Yukawa can produce sizeable charged lepton flavor violation, we examine how large deviation in the neutrino Dirac Yukawa matrix is allowed by present and forthcoming charged lepton flavor violation experiments.
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dc.description.tableofcontentsAbstract
Chapter 1 Introduction 1
Chapter 2 The Standard Model 5
2.1 Electroweak Symmetry Breaking . . . . . . . . . . . . . . . . . . 6
2.2 Flavor Observables and GIM mechanism . . . . . . . . . . . . . . 9
2.3 Gauge Hierarchy Problem and Naturalness . . . . . . . . . . . . 11
Chapter 3 Supersymmetry 16
3.1 Resolving the Hierarchy Problem by Supersymmetry . . . . . . . 16
3.2 The Minimal Supersymmetric Standard Model . . . . . . . . . . 20
Chapter 4 Neutrino Assisted Gauge Mediation Motivation 27
4.1 Soft terms generated from right-handed neutrino messengers . . . 32
4.2 Higgs mass and superparticle spectrum . . . . . . . . . . . . . . . 37
Chapter 5 The Flavon Model Building 48
5.1 Flavon Model Building Motivation . . . . . . . . . . . . . . . . . 48
5.2 Flavon Superpotential Stability . . . . . . . . . . . . . . . . . . . 53
Chapter 6 Charged Lepton Flavor Violation 58
6.1 Yukawa Structure For Neutrino Experiments . . . . . . . . . . . 63
6.2 cLFV of NAGM . . . . . . . . . . . . . . . . . . . . . . . . . . . 67
6.3 lj → liγ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 71
6.4 l?j → l?i l?i l+ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 74
6.5 μ ? e conversion . . . . . . . . . . . . . . . . . . . . . . . . . . . 75
6.6 Correlation between Muon g ? 2, θ13, cLFV and the Higgs . . . 76
Chapter 7 Conculsion 82
Bibliography 84
초록 91
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dc.format.extentvii, 91-
dc.language.isoeng-
dc.publisher서울대학교 대학원-
dc.subjectHiggs boson, supersymmetry, flavor physics, discrete symmetry, neutrino-
dc.subject.ddc523-
dc.titleBeyond The Standard Model Explanations To Flavor Observables-
dc.title.alternative맛깔 관측량에 대한 표준 모형 너머의 설명-
dc.typeThesis-
dc.typeDissertation-
dc.contributor.department자연과학대학 물리·천문학부-
dc.description.degreeDoctor-
dc.date.awarded2015-08-
dc.identifier.holdings000000000023▲000000000025▲000000067464▲-
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