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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/123456789/64301
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor張寶棣
dc.contributor.authorRuei-Jhu Lien
dc.contributor.author李蕊竹zh_TW
dc.date.accessioned2021-06-16T17:39:34Z-
dc.date.available2012-08-17
dc.date.copyright2012-08-17
dc.date.issued2012
dc.date.submitted2012-08-14
dc.identifier.citation[1] Peter W. Higgs, Phys. Rev. Lett. 13, 508–509 (1964).
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[4] B. Aubert et al. (BABAR Collaboration), Phys. Rev. Lett. 103, 081803 (2009).
[5] B. Aubert et al. (BABAR Collaboration), Phys. Rev. Lett. 103, 181801 (2009).
[6] D. J. Lange, Nucl. Instrum. Methods Phys. Res. Sect. A462, 152 (2001).
[7] S. Jadach, B.F.L. Ward, and Z. Was, Comput.Phys.Commun. 130, 260–325 (2000).
[8] R. Brun et al., GEANT 3.21, CERN Report DD/EE/84-1 (1984).
[9] Kenji Inami, Belle Note 629 (2003).
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(1998).
[12] Fredrik Tegenfeldt, http://code.google.com/p/polepp/source/checkout.
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[15] H. W Kim, M. Nakao, S. Nishida, H. Ikeda, Y. Ushiroda, and R. S. Lu, Belle Note 499 (2002).
[16] L. Hinz, Belle Note 954 (2006).
[17] http://pdg.lbl.gov/2012/tables/rpp2012-tab-mesons-b-bbar.pdf.
[18] http://pdg.lbl.gov/2012/tables/rpp2012-sum-leptons.pdf.
[19] Makoto Kobayashi, Yoshihito Iwasaki, Masaru Tada, Norikazu Yamada, Kaoru Iwano, Naoya Torikai, Ryosuke Kadono, Masafumi Tawada, Tsuyoshi Suwada, Takako Miura, Akihiro Bessho, Kotaro (Chief editor) Shibata, and Norihiko Kamikubota, “Anual report 2004” (2004), ISSN 1334-1299.
[20] S. Kurokawa and E. Kikutani, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 499, 1, 1 – 7 (2003).
[21] K. Akai, N. Akasaka, A. Enomoto, J. Flanagan, H. Fukuma, Y. Funakoshi, K. Furukawa, T. Furuya, J. Haba, S. Hiramatsu, K. Hosoyama, T. Ieiri, N. Iida, H. Ikeda, S. Kamada, T. Kamitani, S. Kato, M. Kikuchi, E. Kikutani, H. Koiso, S. Kurokawa, M. Masuzawa, T. Matsumoto, T. Mimashi, T. Mitsuhashi, T.T. Nakamura, Y. Ogawa, K. Ohmi, Y. Ohnishi, S. Ohsawa, N. Ohuchi, K. Oide, E. Perevedentsev, K. Satoh, M. Suetake, Y. Suetsugu, T. Suwada, M. Tawada, M. Tejima, M. Tobiyama, S. Uno, Y. Wu, N. Yamamoto, M. Yoshida, M. Yoshioka, S. Yoshimoto, and F. Zimmermann, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 499, 1, 191 – 227 (2003).
[22] A. Abashian et al., Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 479, 1, 117 – 232 (2002).
[23] H. Aihara et al., Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 568, 1, 269 – 273 (2006), ISSN 0168-9002.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/64301-
dc.description.abstract本篇論文為尋找輕質量希格斯波色子(A0 )的存在證據。實
驗地點位於日本高能加速機構,使用了158百萬個Υ(2S)。根據
次最小超對稱模型(NMSSM)的預測,輕質量希格斯波色子可藉
由衰變通道: Υ(2S) → γA0 以及 Υ(2S) → Υ(1S)π + π − ; Υ(1S) →
γA0 產生。我們的研究包括 A0 → μ+ μ− 和 A0 → τ + τ − 的結果。
由於並未找到輕質量希格斯波色子的存在證據,我們給予90%信
心水準的衰變機率乘積的上限:
B(Υ(2S) → γA0 ) × B(A0 → μ+ μ− ) = (0.02 − 3.11) × 10−6 in the mass range 0.214 ≤ mA0 ≤ 9.00
B(Υ(2S) → γA0 ) × B(A0 → τ + τ − ) = (1.22 − 16.46) × 10−5 in the mass range 3.59 ≤ ma0 ≤ 9.19
B(Υ(1S) → γA0 ) × B(A0 → μ+ μ− ) = (0.005 − 3.54) × 10−6 in the mass range 0.212 ≤ mA0 ≤ 9.0
B(Υ(1S) → γA0 ) × B(A0 → τ + τ − ) = (5.06 − 64.68) × 10−5 in the mass range 3.59 ≤ mA0 ≤ 9.16
zh_TW
dc.description.abstractWe report search for a light Higgs boson (A0 ) using 158 mil
lion Υ(2S) events collected with the Belle detector in the KEKB e+ − e− collider. The Higgs boson is identified in the decays Υ(2S) → γA0 and Υ(2S) → Υ(1S)π + π − , Υ(1S) → γA0 . Results from both A0 → μ+ μ− and A0 → τ + τ − decays are presented. We did not find evidence for the existence of A0 , the 90% C.L. upper limit on the product of braching fractions is given:
B(Υ(2S) → γA0 ) × B(A0 → μ+ μ− ) = (0.02 − 3.11) × 10−6 in the mass range 0.214 ≤ mA0 ≤ 9.00
B(Υ(2S) → γA0 ) × B(A0 → τ + τ − ) = (1.22 − 16.46) × 10−5 in the mass range 3.59 ≤ ma0 ≤ 9.19
B(Υ(1S) → γA0 ) × B(A0 → μ+ μ− ) = (0.005 − 3.54) × 10−6 in the mass range 0.212 ≤ mA0 ≤ 9.0
B(Υ(1S) → γA0 ) × B(A0 → τ + τ − ) = (5.06 − 64.68) × 10−5 in the mass range 3.59 ≤ mA0 ≤ 9.16
en
dc.description.provenanceMade available in DSpace on 2021-06-16T17:39:34Z (GMT). No. of bitstreams: 1
ntu-101-R98222023-1.pdf: 69022965 bytes, checksum: 3aadf3a1f42e7bb7cb7f8bd1fae0960d (MD5)
Previous issue date: 2012
en
dc.description.tableofcontents1 Introduction 1
1.1 Motivation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
1.2 Analysis Strategy . . . . . . . . . . . . . . . . . . . . . . . . . 2
1.3 Data Sample and Monte Carlo Simulation . . . . . . . . . . . 3
2 Event Selection 5
2.1 Skim Criteria . . . . . . . . 5
2.2 Track Selection . . . . . . . 7
2.3 Particle Identification . . . . 7
2.4 Additional Selection of Each Mode . . 8
2.5 Best Candidate . . . . . . . 9
2.6 Backgrounds . . . . . . . . . 9
3 Signal Extraction. . . .14
3.1 γμ+ μ− , γτ + τ − (τ τ → eμ) , π + π − γμ+ μ− with mμμ>3.1 GeV
and π + π − γτ + τ − (τ τ → eμ) events . . . . . .14
3.1.1 γμ+ μ− event . . . . . . . . . . . . . .18
3.1.2 γτ + τ − (τ τ → eμ) event . . . . . . . .20
3.1.3 π + π − γμ+ μ− event . . . . . . . . . . .22
3.1.4 π + π − γτ + τ − (τ τ → eμ) event . . . . .24
3.2 π + π − γμ+ μ− event with mμμ < 3.1 GeV . . .25
4 Correction Factors and Uncertainties 27
5 Results 33
6 Conclusion 36
A Belle Experiment 39
A.1 KEKB Accelerator . . . . . . . . . . . . . . . . . . . . . . . . 39
A.2 Belle Detector . . . . . . . . . . . . . . . . . . . . . . . . . . . 43
A.3 Beam Pipe . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43
A.4 Silicon Vertex Detector (SVD) . . . .45
A.5 Central Drift Chamber (CDC) . . . .46
A.6 Aerogel ~Cerenkov Counter (ACC) . .47
A.7 Time of Flight Counter (TOF) . . . .47
A.8 Electromagnetc Calorimeter (ECL) .48
A.9 Extreme Forward Calorimeter (EFC)49
A.10 KL and Muon Detector (KLM) . . .49
B Details of Setting Event Selections 52
B.1 γμ+ μ− event . . . . . . . . . . . .52
B.2 γτ + τ − (τ τ → eμ) event . . . . . .53
B.3 π + π − γμ+ μ− event . . . . . . . . .55
B.4 π + π − γτ + τ − (τ τ → eμ) event . . .57
dc.language.isoen
dc.subject希格斯粒子zh_TW
dc.subject(2S)zh_TW
dc.subjectlight Higgs bosonen
dc.subject(2S)en
dc.titleϒ(2S)衰變至希格斯粒子之探尋zh_TW
dc.titleSearch for a light Higgs boson in ϒ(2S) decayen
dc.typeThesis
dc.date.schoolyear100-2
dc.description.degree碩士
dc.contributor.oralexamcommittee王名儒,侯維恕,熊怡
dc.subject.keyword希格斯粒子,&#978,(2S),zh_TW
dc.subject.keywordlight Higgs boson,&#978,(2S),en
dc.relation.page57
dc.rights.note有償授權
dc.date.accepted2012-08-15
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept物理研究所zh_TW
顯示於系所單位:物理學系

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