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  1. NTU Theses and Dissertations Repository
  2. 理學院
  3. 物理學系
Please use this identifier to cite or link to this item: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/27493
Full metadata record
???org.dspace.app.webui.jsptag.ItemTag.dcfield???ValueLanguage
dc.contributor.advisor熊怡(Yee Hsiung)
dc.contributor.authorMeng-Lin Wuen
dc.contributor.author吳孟霖zh_TW
dc.date.accessioned2021-06-12T18:07:06Z-
dc.date.available2008-01-02
dc.date.copyright2008-01-02
dc.date.issued2007
dc.date.submitted2007-12-27
dc.identifier.citation[1] HyperCP Collaboration, H. Park et al., Evidence for the decay
Sigma+ ! p mu+ mu-,' Phys. Rev. Lett. 94 (2005) 021801,
hep-ex/0501014.
[2] D. S. Gorbunov and V. A. Rubakov, On sgoldstino interpretation of
HyperCP events,' Phys. Rev. D73 (2006) 035002, hep-ph/0509147.
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collider searches,' Nucl. Phys. B602 (2001) 213{237, hep-ph/0007325.
[4] D. S. Gorbunov and V. A. Rubakov, Kaon physics with light
sgoldstinos and parity conservation,' Phys. Rev. D64 (2001) 054008,
hep-ph/0012033.
[5] X.-G. He, J. Tandean, and G. Valencia, Has HyperCP observed a light
Higgs boson?,' Phys. Rev. Lett. 98 (2007) 081802, hep-ph/0610362.
[6] KTeV Collaboration, A. Alavi-Harati et al., Measurement of the
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917{921, hep-ex/9902029.
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hep-ex/0205010.
[8] Particle Data Group Collaboration, W. M. Yao et al., Review of
particle physics,' J. Phys. G33 (2006) 1{1232.
[9] T. Inagaki et al., Measurement of the K0L
! 0 ,' Proposal TN001
(1996).
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anti-nu decay at the KEK 12-GeV proton synchrotron,' Nucl.
Instrum. Meth. A545 (2005) 542{553.
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nu anti-nu experiment at KEK-PS,' Nucl. Instrum. Meth. A545
(2005) 278{295.
[12] M. Doroshenko, Calibration of E391a detector,'. TN171.
[13] K. Sakashita, Search for the decay KL ! 0 . PhD thesis, 2006.
[14] S. Ajimura et al., Measurement of the photon detection ine ciency of
electromagnetic calorimeters at energies below 1-GeV,' Nucl. Instrum.
Meth. A552 (2005) 263{275.
[15] Y. Akune, Performance of the Main Barrel,' Master's thesis, 2004.
[16] H. Watanabe. PhD thesis, 2002.
[17] M. Yamaga, DAQ system at the Engineering Run on 2002 for
KEK-PS E391a experiment, etc,'. TN148.
[18] C. A. S. Group, GEANT-Detector Description and Simulation Tool,'
CERN W5013 (1993).
[19] G. Perdue, MC Tuning and Six Cluster Events,'. Technote Draft.
[20] G. D'Ambrosio and J. Portoles, Vector meson exchange contributions
to K ! pi gamma gamma and K(L) ! gamma l+ l-,' Nucl. Phys.
B492 (1997) 417{454, hep-ph/9610244.
[21] H. S. Lee, CsI Angle and Energy correction,' Meeting slides (Aug,
2005).
[22] J. Conrad, O. Botner, A. Hallgren, and C. Perez de los Heros,
Including systematic uncertainties in con dence interval construction
for Poisson statistics,' Phys. Rev. D67 (2003) 012002, hep-ex/0202013
[23] G. J. Feldman and R. D. Cousins, A Uni ed approach to the classical
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3873{3889, physics/9711021.
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[25] P. Avery, Fitting Theory I { V.'
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Polarization in b ! s Transitions at Belle. PhD thesis, National
Taiwan University, 2005.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/27493-
dc.description.abstract本論文尋找可能的中性K介子衰變至pi0介子以及輕準純量
sgoldstino(代稱X粒子)。所使用數據來自日本國家高能加速器
中心質子加速器的E391a 偵測器,於九十四年二月至三月間取
得。
經由事例重建,我們針對四組可能的質量範圍搜尋,並無發
現顯著訊號,因此給予90%信心水準之衰變分率上限,分別為
Br(KL->pi0X(181.7 MeV)) < 2.26e-6
Br(KL->pi0X(198.0 MeV)) < 1.97e-6
Br(KL->pi0X(214.3 MeV)) < 1.81e-6
Br(KL->pi0X(230.6 MeV)) < 1.17e-6
zh_TW
dc.description.abstractWith mX = 214.3 MeV as hinted by a previous HyperCP
experiment, we report the first search of the decay KL->pi0X
using the Run2 data sample recorded with the E391a detector
at KEK-PS. The particle X has a theoretical interpretation as
the pseudoscalar sgoldstino. It is predicted to decay
predominantly to two photons. As a result of this search, we
set a 90% confidence-level upper limit for its branching
ratio at B(KL->pi0X)<1.81e-6. We also performed a search for
the same mode assuming different mX: 181.7MeV, 198MeV,
230.6MeV and set respective 90% confidence-level upper
limits: B(KL->pi0X181.7)<2.26e-6,
B(KL->pi0X198.0)<1.97e-6 and B(KL->pi0X230.6)<1.17e-6. The
KL flux for the E391a Run2 data set is also measured to be (4.83+-0.21)e9 in the fiducial region.
en
dc.description.provenanceMade available in DSpace on 2021-06-12T18:07:06Z (GMT). No. of bitstreams: 1
ntu-96-R94222025-1.pdf: 4403180 bytes, checksum: 41b23023e62c09ada07f0d44d693fe45 (MD5)
Previous issue date: 2007
en
dc.description.tableofcontentsIntroduction 1
1.1 The X particle - HyperCP experiment . . . . . . . . . . . . . 1
1.2 The sgoldstino interpretation . . . . . . . . . . . . . . . . . . 1
1.3 The Higgs boson interpretation . . . . . . . . . . . . . . . . . 4
1.4 Hints at decay K0L
! 0X(X !
) - KTeV and NA48 experiments
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
1.5 K mesons . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
1.6 Thesis outline . . . . . . . . . . . . . . . . . . . . . . . . . . . 7
2 KEK E391a 8
2.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8
2.2 The Neutral Beam . . . . . . . . . . . . . . . . . . . . . . . . 8
2.2.1 Particle Generation . . . . . . . . . . . . . . . . . . . . 8
2.2.2 The Pencil Beam . . . . . . . . . . . . . . . . . . . . . 9
2.3 The E391a Detector . . . . . . . . . . . . . . . . . . . . . . . 10
2.3.1 Electromagnetic Calorimeter . . . . . . . . . . . . . . . 11
2.3.2 Charged Veto . . . . . . . . . . . . . . . . . . . . . . . 14
2.3.3 Main Barrel . . . . . . . . . . . . . . . . . . . . . . . . 17
2.3.4 Front Barrel . . . . . . . . . . . . . . . . . . . . . . . . 21
2.3.5 Collar Counters . . . . . . . . . . . . . . . . . . . . . . 22
2.3.6 Back Anti . . . . . . . . . . . . . . . . . . . . . . . . . 24
2.3.7 Beam Hole Charged Veto . . . . . . . . . . . . . . . . . 25
2.4 Vacuum System . . . . . . . . . . . . . . . . . . . . . . . . . . 25
2.4.1 Overview . . . . . . . . . . . . . . . . . . . . . . . . . 27
2.4.2 PMT operation in vacuum . . . . . . . . . . . . . . . . 27
2.5 Triggering . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 29
2.5.1 AmpDiscri module . . . . . . . . . . . . . . . . . . . . 29
2.5.2 Physics trigger . . . . . . . . . . . . . . . . . . . . . . 29
2.5.3 Other triggers . . . . . . . . . . . . . . . . . . . . . . . 32
2.5.4 Data Acquisition . . . . . . . . . . . . . . . . . . . . . 33
2.6 Data Sample . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33
2.6.1 Data taking shifts . . . . . . . . . . . . . . . . . . . . . 34
3 Monte Carlo Simulation 36
3.1 Particle generation . . . . . . . . . . . . . . . . . . . . . . . . 36
3.2 KL propagation and decay . . . . . . . . . . . . . . . . . . . . 37
3.3 Decay modes and statistics . . . . . . . . . . . . . . . . . . . . 37
3.3.1 Statistics . . . . . . . . . . . . . . . . . . . . . . . . . . 38
3.4 Energy deposit . . . . . . . . . . . . . . . . . . . . . . . . . . 38
3.5 Accidental activity . . . . . . . . . . . . . . . . . . . . . . . . 40
3.6 Combination of modes . . . . . . . . . . . . . . . . . . . . . . 40
4 Analysis Method 41
4.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . 41
4.2 Event Reconstruction . . . . . . . . . . . . . . . . . . . . . . . 42
4.2.1 Clustering routine . . . . . . . . . . . . . . . . . . . . . 42
4.2.2 Kinematic reconstruction . . . . . . . . . . . . . . . . . 43
4.2.3 Reconstruction results . . . . . . . . . . . . . . . . . . 52
4.3 Candidate Selection . . . . . . . . . . . . . . . . . . . . . . . . 52
4.3.1 Signal box . . . . . . . . . . . . . . . . . . . . . . . . . 52
4.3.2 0 region . . . . . . . . . . . . . . . . . . . . . . . . . . 53
4.4 Background Suppression . . . . . . . . . . . . . . . . . . . . . 53
4.4.1 Veto cuts . . . . . . . . . . . . . . . . . . . . . . . . . 54
4.4.2 Kinematic and MB cuts . . . . . . . . . . . . . . . . . 56
4.4.3 Cluster quality . . . . . . . . . . . . . . . . . . . . . . 60
4.4.4 0 tail . . . . . . . . . . . . . . . . . . . . . . . . . . . 63
4.4.5 KL radius at the exit of collimator 6 . . . . . . . . . . 63
4.4.6 Selection results . . . . . . . . . . . . . . . . . . . . . . 63
5 Signal Extraction 66
5.1 Likelihood Method . . . . . . . . . . . . . . . . . . . . . . . . 66
5.1.1 Denition . . . . . . . . . . . . . . . . . . . . . . . . . 66
5.1.2 Background PDF . . . . . . . . . . . . . . . . . . . . . 67
5.1.3 Background normalization . . . . . . . . . . . . . . . . 69
5.1.4 Signal PDF . . . . . . . . . . . . . . . . . . . . . . . . 70
5.1.5 Fit results . . . . . . . . . . . . . . . . . . . . . . . . . 70
Upper Limit Estimation . . . . . . . . . . . . . . . . . . . . . 71
5.2.1 Systematic error study . . . . . . . . . . . . . . . . . . 71
5.2.2 Implementation of systematic errors . . . . . . . . . . . 75
5.2.3 Final tting results . . . . . . . . . . . . . . . . . . . . 75
5.3Counting Method . . . . . . . . . . . . . . . . . . . . . . . . . 77
5.4KL Flux . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 78
Conclusions and Prospects 81
6.1Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . 81
6.2Prospects . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 82
6.2.1 Increased data statistics { Run3 data set . . . . . . . . 82
6.2.2 Increased MC statistics . . . . . . . . . . . . . . . . . . 83
6.2.3 Finer CsI crystals { E14 experiment . . . . . . . . . . . 84
! 0
Monte Carlo 89
Kinematic Fitting 92
dc.language.isoen
dc.subject準純量sgoldstinozh_TW
dc.subjectK介子zh_TW
dc.subject衰變zh_TW
dc.title尋找中性K介子衰變至準純量sgoldstino粒子zh_TW
dc.titleSearch for KL decay to light pseudoscalar sgoldstino at E391aen
dc.typeThesis
dc.date.schoolyear96-1
dc.description.degree碩士
dc.contributor.oralexamcommittee王名儒(Min-Zu Wang),張寶棣(Pao-Ti Chang),何小剛(Xiao-Gang He)
dc.subject.keywordK介子,衰變,準純量sgoldstino,zh_TW
dc.subject.keywordKL decay,sgoldstino,E391a,en
dc.relation.page88
dc.rights.note有償授權
dc.date.accepted2007-12-27
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept物理研究所zh_TW
Appears in Collections:物理學系

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