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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/123456789/72270
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor張寶棣
dc.contributor.authorYu-Chieh Kuen
dc.contributor.author辜禹傑zh_TW
dc.date.accessioned2021-06-17T06:32:27Z-
dc.date.available2018-08-21
dc.date.copyright2018-08-21
dc.date.issued2018
dc.date.submitted2018-08-16
dc.identifier.citation[1] ”CKM group wiki page ”. URL:http://belle.kek.jp/secured/wiki/doku.php?id=physics:ckm:htag.
[2] ”Elementary Particle Interaction(Wikipedia)”.
URL:https://en.wikipedia.org/wiki/Standard_Model#/media/File:Elementary_particle_interactions_in_the_Standard_Model.png.
[3] J. Conradet al. ”Including systematic uncertainties in confidence interval construction for Poisson statistics”. PHYSICAL REVIEW D, 67, 2003.
[4] A. Badin and A. A. Petrov. ”Searching for light Dark Matter in heavy meson decays”. Phys. Rev. D, 82, 2010.
[5] G. Buchalla and A. J. Buras. ”QCD corrections to rare K- and B-decays for arbitrary top quark mass”. Nuclear Physics B, 400(1-3):225–239,1993.
[6] Da-Xin Zhang Cai-Dian Lü. ”B S (B d ) → ν ν̄γ”. PHYSICS LETTERS B, pages 348–352, 1996.
[7] Athanasios Dedes and Herbi Dreiner. ”Attempts at explaining the NuTeV observation of dimuon events”. Phys.Rev. D65, 2001.
[8] A. Abashian et al. ”The Belle detector”. Nucl. Instruments Methods
Phys. Res. Sect, A Accel. spectrometers,Detect.Assoc.Equip., 479.1:117–232, 2002.
[9] J.P. Lees et al. ”Improved Limits on B 0 Decays to Invisible Final States and to ν ν̄γ”. Phys.Rev. D86, 2012.
[10] Michael Feindt et al. “A hierarchical NeuroBayes-based algorithm for full reconstruction of B mesons at B factories”. Nucl. Instruments Methods Phys. Res.Sect. A Accel. Spectrometers, Detect. Assoc. Equip.,654.1:432–440, 2011.
[11] S. Kurokawa et al. ”Overview of the KEKB accelerators”. Nucl. Instruments Methods Phys. Res. Sect, A Accel. spectrometers,Detect. Assoc.Equip., 499.1:1–7, 2003.
[12] L. Hinz. ”Lepton ID efficiency correction and systematic error”. Bellenote 954, 2006.
[13] Chia-Ling Hsu. ”Study of B → invisiblef inalstate”. Bellenote 1159,2012.
[14] Vladimir Kulikovskiy. ”Adding a systematic uncertainty to the signal estimation in the on/off-zone measurements”. arXiv:1303.5195 [stat.AP],2013.
[15] S. Neubauer. “ new full reconstruction tool using NeuroBayes”. Bellenote 1167, 2012.
[16] S. Nishida. ”Study of kaon and pion identification using inclusive D*sample”. Bellenote 779, 2005.
[17] Giovanni Punzi. ”sensitivity of searches for new signals and its optimization”. Conf. Stat. Probl. Part. Physics, Astrophys. Cosmol, page 5,2003.
[18] A. Sibidanov and K. Varvel. ”Exclusive B → πlν B → ρlν and B → ωlν Decays using New Full Reconstruction Tagging”. Bellenote 1206, 2012.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/72270-
dc.description.abstract本篇論文使用了強子標籤法在 Belle 實驗中尋找 B 0 → (γ)νν̅ 之稀有衰變,並借此探討標準模型外的新物理之可能性。本篇論文的實驗數據是由日本高能加速器研究機構 B 介子工廠(KEKB)之 Belle 偵測器在能量不對稱之正負電子對狀器中所蒐集,來自 Υ(4S) 衰變的 771 百萬 B0 B0bar介子對。本篇論文使用了強子標籤法完整重組對狀事件中的一顆 B 介子,並藉著要求剩餘事件中沒有帶電粒子、中性 π 介子 及中性 K 介子,以描述B 0 → (γ)νν̅ 之訊號,本篇論文最終呈現 90%信心水準之下由蒙地卡羅模擬所求得的衰變分支上限值。zh_TW
dc.description.abstractWe perform a study to search for the decays B 0 → ν ν̄ and B 0 → ν ν̄γ using a sample of 771 million B- B̄ pairs collected with the Belle detector on the Υ(4S) resonance at KEK e + e − collider. The two resonance signature is identified by fully reconstructing the accompanying B meson that decays hadronically and requiring no charged particles, neutral pions and neutral kaons in the signal side. The branching fraction upper limits at 90% confidence level is presented.en
dc.description.provenanceMade available in DSpace on 2021-06-17T06:32:27Z (GMT). No. of bitstreams: 1
ntu-107-R05222024-1.pdf: 6447467 bytes, checksum: 6d1805dd78a63e8bc0b20a40ed7c1efb (MD5)
Previous issue date: 2018
en
dc.description.tableofcontentsAbstract iii
1 Introduction 1
1.1 The Standard Model.............................1
1.2 Motivation.....................................2
2 The Belle Experiment 5
2.1 KEKB Accelerator...............................5
2.2 Belle Detector.................................5
2.2.1 Beam Pipe....................................7
2.2.2 Extreme Forward Calorimeter(EFC).............9
2.2.3 Silicon Vertex Detector(SVD)................10
2.2.4 Central Drift Chamber(CDC)..................11
2.2.5 Aerogel Cherenkov counter system(ACC).......13
2.2.6 Time of Flight(TOF).........................14
2.2.7 Electromagnetic Calorimeter(ECL)............16
2.2.8 K L and Muon Detector(KLM)..................17
3 Data Sample 21
3.1 Samples.......................................21
3.2 B 0 → γν ν̄ Model..............................22
4 Selections 24
4.1 Hadronic Tagging and Tag Side Selections......24
4.2 E ECL ........................................24
4.3 cosθ T........................................24
4.4 Photon .......................................25
4.5 Track veto ...................................26
4.6 π 0 veto .....................................27
4.7 K L veto .....................................28
5 Neural Network 30
5.1 Tag side Neural Network ......................30
5.2 Shape variables Neural Network ...............30
5.3 Training Results .............................31
5.4 Two dimensional optimization on FOM ..........34
6 Fitter Construction(B 0 → ν ν̄) 37
6.1 Components ...................................37
6.2 Increase statistics ..........................38
6.3 Off Resonance data ...........................39
6.4 Fitting function .............................42
6.5 Pull test ....................................43
7 Control Sample 50
7.1 Modes and approach............................50
7.2 Particles Identification .....................50
7.3 Event Selections .............................51
7.4 E ECL shape in signal MC .....................52
7.5 Correction factor and systematic error........53
7.6 Control Sample Validity ......................55
8 Upper Limit Estimation 64
8.1 Systematic Uncertainty on Signal Efficiency...64
8.1.1 Full Recon correction on Efficiency.........64
8.1.2 Summary.....................................67
8.2 Counting Method...............................67
8.2.1 Expected Background in box..................68
8.2.2 Upper Limit Estimation......................70
8.3 Fitting Method................................71
8.3.1 Uncertainty of pdf modeling.................73
8.3.2 Upper limit estimation......................74
9 Conclusion 77
10 Appendix 78
10.1 Training variables distribution comparison in each bin ..................................................78
dc.language.isoen
dc.title使用強子標籤法在 Belle 實驗中尋找 B 介子衰變至(γ)νν̅ 之分析zh_TW
dc.titleSearch for B 0 → (γ)νν̅ at Belleen
dc.typeThesis
dc.date.schoolyear106-2
dc.description.degree碩士
dc.contributor.oralexamcommittee王名儒,徐靜戈,張敏娟,王正祥
dc.subject.keywordB介子,稀有B衰變,Belle 實驗,zh_TW
dc.subject.keywordB meson,rare B decay,Belle experiment,en
dc.relation.page81
dc.identifier.doi10.6342/NTU201803480
dc.rights.note有償授權
dc.date.accepted2018-08-16
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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