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  1. NTU Theses and Dissertations Repository
  2. 理學院
  3. 物理學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/66038
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor王名儒(Minzu Wang)
dc.contributor.authorPei-Cheng Luen
dc.contributor.author盧沛成zh_TW
dc.date.accessioned2021-06-17T00:19:49Z-
dc.date.available2020-03-03
dc.date.copyright2020-03-03
dc.date.issued2020
dc.date.submitted2020-02-12
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/66038-
dc.description.abstract日本筑波KEK之B工廠(包括了KEKB 加速器以及BELLE 偵測器) 於1998 至2010 年間收集了772 百萬BB 介子對實驗數據,藉著準確的粒子分辨率以及粒子的四動量,我們使用了這些BB 介子對,量測了B+衰變至pΛK+K− 以及B+ 衰變至pΛK+K+ 四體衰變分支比及中間態衰變分支比。藉由分析各中間態的量測,我們能夠更清楚了解此衰變的結構。在此量測中,我們發現了四個新衰變態: genuine fourbody decay of B(B+ → pΛK+K−) = (4.10+0.45−0.43± 0.50)×10−6、genuine fourbody decay of B(B+ → pΛK+K+) = (3.70+0.39−0.37±0.44)×10−6、B(B+ → pΛϕ) = (7.95±2.09±0.77) × 10−7 and B(ηc → p¯ΛK− +c.c.) = (2.83+0.36−0.34± 0.35) × 10−3 )。這裡B指的是粒子的衰變分支比。根據我們對Λ−c 的了解,Λ−c 為udc 態,Λ−c 與Λ 皆為IJP = 0(1/2+),以上量測與B(B0 → p¯Λ−c π+π−) > B(B+ → p¯Λ−c π+)的衰變分支比結構類似。新的魅粒子態也同時被發現,可根據此實驗結果對於魅粒子態有更進一步的了解。zh_TW
dc.description.abstractFrom 1998 to 2010, the B factory (including KEKB accelerator and BELLE detector)at KEK collected 772 million BB pairs. With the precise identification and measurement of four-momentum of particles, we finished the studies: genuine four-body decay of B(B+ → pΛK+K−) = (4.10+0.45−0.43± 0.50)×10−6、genuine four-body-decay of B(B+ → pΛK+K+) = (3.70+0.39−0.37± 0.44)×10−6、B(B+ →pΛϕ) = (7.95 ± 2.09 ± 0.77) × 10−7 and B(ηc → p¯ΛK− +c.c.) = (2.83+0.36−0.34±0.35) × 10−3. Here B is the branching fraction of the particles. According to our understanding of Λ−c , Λ−c is udc state, Λ−c and Λ are IJP = 0(1/2+). The hierarchical structure seems to exist, e.g., B(B0 → p¯Λ−c π+π−) > B(B+ → p¯Λ−c π+).
We also found a new charmonium decay mode, ηc → p¯ΛK− +c.c., which can be compared with the measured decay mode, J/ψ → p¯ΛK− +c.c., thus we could have a clearer understanding on charmonium system.
en
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dc.description.tableofcontents1 Introduction 1
1.1 Motivation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
1.2 Standard Model . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
1.2.1 Mesons and Baryons . . . . . . . . . . . . . . . . . . . . 3
1.2.2 B Physics . . . . . . . . . . . . . . . . . . . . . . . . . . 6
1.2.3 The Cabibbo-Kobayashi-Maskawa Matrix . . . . . . . . . 7
1.2.4 CP violation . . . . . . . . . . . . . . . . . . . . . . . . 9
2 Belle Experiment 11
2.1 KEKB BFactory. . . . . . . . . . . . . . . . . . . . . . . . . . 11
2.2 BELLE Detector . . . . . . . . . . . . . . . . . . . . . . . . . . 13
2.2.1 Beamline
Magnets near the IP and Beam Pipe . . . . . . 18
2.2.2 Extreme Forward Calorimeter (EFC) . . . . . . . . . . . 18
2.2.3 Silicon Vertex Detector (SVD) . . . . . . . . . . . . . . . 21
2.2.4 Central Drift Chamber (CDC) . . . . . . . . . . . . . . . 22
2.2.5 Aerogel Čerenkov Counter System (ACC) . . . . . . . . . 24
2.2.6 TimeofFlight Counters (TOF) . . . . . . . . . . . . . . 26
2.2.7 Electromagnetic Calorimeter (ECL) . . . . . . . . . . . . 29
2.2.8 Particle Identification of Electrons and Charged Kaons,
EID and KID . . . . . . . . . . . . . . . . . . . . . . . . 31
2.2.9 KL and Muon Detection System (KLM) . . . . . . . . . . 32
3 Introduction 35
3.1 B Reconstruction and Event Selection . . . . . . . . . . . . . . . 35
3.2 Charged Track Selection . . . . . . . . . . . . . . . . . . . . . . 35
3.3 Λ Reconstruction . . . . . . . . . . . . . . . . . . . . . . . . . . 36
3.4 Best Candidate Selection . . . . . . . . . . . . . . . . . . . . . . 36
3.5 D0 and D∗0 veto . . . . . . . . . . . . . . . . . . . . . . . . . . 36
3.6 Signal Monte Carlo(MC) . . . . . . . . . . . . . . . . . . . . . . 36
3.7 Selections Summary . . . . . . . . . . . . . . . . . . . . . . . . 37
3.8 Possible Modes . . . . . . . . . . . . . . . . . . . . . . . . . . . 38
4 Background Study 39
4.1 Overview of Backgrounds Study . . . . . . . . . . . . . . . . . . 39
4.2 Continuum Suppression . . . . . . . . . . . . . . . . . . . . . . . 39
4.2.1 ΔZ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 39
4.2.2 cosθB . . . . . . . . . . . . . . . . . . . . . . . . . . . . 40
4.2.3 Kakuno Super FoxWolfram(
KSFW) . . . . . . . . . . . 40
4.2.4 q × r . . . . . . . . . . . . . . . . . . . . . . . . . . . . 42
4.3 Best FOM . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 42
4.4 BB Background . . . . . . . . . . . . . . . . . . . . . . . . . . 44
5 Study of Intermediate States 47
5.1 B+ → pΛK+K− . . . . . . . . . . . . . . . . . . . . . . . . . . 47
5.2 B+ → pΛK+K+ . . . . . . . . . . . . . . . . . . . . . . . . . . 48
5.3 Issue of Dibaryonic Threshold Enhancement . . . . . . . . . . . . 49
6 2D Fitting of Data 51
6.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51
6.2 2D Fitter . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 54
6.3 Measurement of Inclusive Decay . . . . . . . . . . . . . . . . . . 56
6.4 Fourbody
Decay . . . . . . . . . . . . . . . . . . . . . . . . . . 58
7 Fitting of Data for Resonance Modes 61
7.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61
7.2 3D Fitter and 4D Fitter . . . . . . . . . . . . . . . . . . . . . . . 64
7.3 Results of Fitting . . . . . . . . . . . . . . . . . . . . . . . . . . 68
7.3.1 (B+ → J/ψK+) × (inclusive J/ψ → pΛK−) . . . . . . 71
7.3.2 (B+ → ηcK+) × (inclusive ηc → pΛK−) . . . . . . . . 71
7.3.3 (B+ → χc1K+) × (inclusive χc1 → pΛK−) . . . . . . . 73
7.3.4 (B+ → pΛϕ) × (ϕ → K+K−) . . . . . . . . . . . . . . 75
7.3.5 (B+ → Λ(1520)ΛK+) × (Λ(1520) → pK−) . . . . . . . 77
7.3.6 (B+ → ηcK+) × (ηc → Λ(1520)Λ) × (Λ(1520) → pK−) 79
7.3.7 (B+ → J/ψK+) × (J/ψ → Λ(1520)Λ) × (Λ(1520) →
pK−) . . . . . . . . . . . . . . . . . . . . . . . . . . . . 79
7.3.8 (B+ → Λ(1520)ΛK+) × (Λ(1520) → pK+) . . . . . . . 81
8 Conclusion 83
8.1 Summary of Measured Branching Fractions . . . . . . . . . . . . 83
8.2 Decay Process of Dibaryonic System . . . . . . . . . . . . . . . . 83
9 Systematic Error Study 85
9.1 Tracking Uncertainty . . . . . . . . . . . . . . . . . . . . . . . . 85
9.2 Number of B ¯B Pairs Uncertainty . . . . . . . . . . . . . . . . . . 85
9.3 Dibaryonic system(X””bb) Uncertainty in MC . . . . . . . . . . . 85
9.4 Proton Identification Uncertainty . . . . . . . . . . . . . . . . . . 87
9.5 Kaon Identification Uncertainty . . . . . . . . . . . . . . . . . . 87
9.6 Signal PDF(ΔE, Mbc and Mres) Uncertainty . . . . . . . . . . . . 87
9.7 MC Efficiency Uncertainty . . . . . . . . . . . . . . . . . . . . . 90
9.8 qq Suppression Uncertainty . . . . . . . . . . . . . . . . . . . . . 91
9.9 Λ Selection Uncertainty . . . . . . . . . . . . . . . . . . . . . . . 93
9.10 D0 and D∗0 veto Uncertainty . . . . . . . . . . . . . . . . . . . . 93
9.11 Summary of Systematic Errors . . . . . . . . . . . . . . . . . . . 94
A Signal MC Efficiencies with Each Cut 97
A.1 B+ → pΛK+K− . . . . . . . . . . . . . . . . . . . . . . . . . . 97
A.2 B+ → pΛK+K+ . . . . . . . . . . . . . . . . . . . . . . . . . . 102
B Plots of Variables for qq Suppression 107
B.1 B+ → pΛK+K− . . . . . . . . . . . . . . . . . . . . . . . . . . 107
B.2 B+ → pΛK+K+ . . . . . . . . . . . . . . . . . . . . . . . . . . 112
C Spectra of Invariant Mass 117
C.0.1 B+ → pΛK+K− . . . . . . . . . . . . . . . . . . . . . . 117
C.0.2 B+ → pΛK+K+ . . . . . . . . . . . . . . . . . . . . . . 123
C.0.3 Combined Data . . . . . . . . . . . . . . . . . . . . . . . 127
D Signal Monte Carlo-PHSP 129
E Signal Monte Carlo-Xbb 131
F Efficiency Corrections 133
F.1 Kaon ID Efficiency Correction(εkID) . . . . . . . . . . . . . . . . 133
F.2 Proton ID Efficiency Correction(εpID) . . . . . . . . . . . . . . . 136
G Models of Resonance Mass 139
H Plots of Xbb distribution 141
I Float Variables in Fitting for Resonance Modes 145
J 2D Trigger Maintenance at BELLE II 147
J.1 BELLE II Detector . . . . . . . . . . . . . . . . . . . . . . . . . 147
J.2 Level 1 Trigger System in BELLE II Experiment . . . . . . . . . 148
J.3 The connection between boards . . . . . . . . . . . . . . . . . . . 148
J.4 Early Check of 2D Data . . . . . . . . . . . . . . . . . . . . . . . 149
J.5 The Updating of 2D Firmware . . . . . . . . . . . . . . . . . . . 152
J.6 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 152
dc.language.isoen
dc.subjectB介子衰變zh_TW
dc.subject魅子中間態zh_TW
dc.subject雙重子衰變zh_TW
dc.subjectDecay of B mesonen
dc.subjectIntermediate decay of charmoniumen
dc.subjectDibaryonic decayen
dc.titleB+ 介子衰變至p Λ-bar K+ K−以及p-bar Λ K+ K+ 之分析zh_TW
dc.titleB+ decaying to p Λ-bar K+ K− and p-bar Λ K+ K+en
dc.typeThesis
dc.date.schoolyear108-1
dc.description.degree博士
dc.contributor.oralexamcommittee張寶棣(Pao-Ti Chang),王正祥(Chung-Hsiang Wang),徐靜戈(Jing-Ge Shui),張敏娟(Ming-Juan Chang)
dc.subject.keywordB介子衰變,雙重子衰變,魅子中間態,zh_TW
dc.subject.keywordDecay of B meson,Dibaryonic decay,Intermediate decay of charmonium,en
dc.relation.page157
dc.identifier.doi10.6342/NTU202000406
dc.rights.note有償授權
dc.date.accepted2020-02-13
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept物理學研究所zh_TW
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