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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/123456789/87168
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor呂榮祥zh_TW
dc.contributor.advisorRong-Shyang Luen
dc.contributor.author郭晉嘉zh_TW
dc.contributor.authorChin-Chia Kuoen
dc.date.accessioned2023-05-18T16:08:32Z-
dc.date.available2023-11-09-
dc.date.copyright2023-05-10-
dc.date.issued2023-
dc.date.submitted2023-02-15-
dc.identifier.citation[1] CMS Collaboration. The Phase-2 Upgrade of the CMS Tracker. Tech. rep. Geneva: CERN, 2017. doi: 10.17181/CERN.QZ28.FLHW. url: https://cds.cern.ch/record/2272264.
[2] CMS Collaboration. The CMS electromagnetic calorimeter project: Technical Design Report. Technical design report. CMS. Geneva: CERN, 1997. url: https://cds.cern.ch/record/349375.
[3] CMS Collaboration. CMS Technical Design Report for the Phase 1 Upgrade of the Hadron Calorimeter. Tech. rep. Additional contact persons: Jeffrey Spalding, Fermilab, spalding@cern.ch, Didier Contardo, Universite Claude Bernard-Lyon I, contardo@cern.ch. 2012. url: https://cds.cern.ch/record/1481837.
[4] CMS Collaboration. “The performance of the CMS muon detector in proton- proton collisions at √s = 7 TeV at the LHC”. In: Journal of Instrumentation 8.11 (Nov. 2013), P11002. doi: 10.1088/1748-0221/8/11/P11002. url: https://dx.doi.org/10.1088/1748-0221/8/11/P11002.
[5] CMS Collaboration. “Particle-flow reconstruction and global event description with the CMS detector”. In: Journal of Instrumentation 12.10 (Oct. 2017), P10003. doi: 10.1088/1748-0221/12/10/P10003. url: https://dx.doi.org/10.1088/1748-0221/12/10/P10003.
[6] CMS Collaboration. The Phase-2 Upgrade of the CMS Endcap Calorimeter. Tech. rep. Geneva: CERN, 2017. doi: 10.17181/CERN.IV8M.1JY2. url: https://cds.cern.ch/record/2293646.
[7] CMS Collaboration. A MIP Timing Detector for the CMS Phase-2 Upgrade. Tech. rep. Geneva: CERN, 2019. url: https://cds.cern.ch/record/2667167.
[8] CMS Collaboration. “Performance of reconstruction and identification of τ leptons decaying to hadrons and ντ in pp collisions at √s=13 TeV”. In: Journal of Instrumentation 13.10 (Oct. 2018), P10005. doi: 10.1088/1748-0221/13/10/ P10005. url: https://dx.doi.org/10.1088/1748-0221/13/10/P10005.
[9] Stefan Gundacker and Arjan Heering. “The silicon photomultiplier: fundamentals and applications of a modern solid-state photon detector”. In: Physics in Medicine & Biology 65.17 (Aug. 2020), 17TR01. doi: 10.1088/1361-6560/ab7b2d. url: https://dx.doi.org/10.1088/1361-6560/ab7b2d.
[10] ACTIVITY BOOK FOR STUDENTS - Alibava Systems. first. 2015.
[11] MICROC-SERIES - Silicon Photomultipliers (SiPM), Low-Noise, Blue-Sensitive. Rev. 9. Feb. 2022.
[12] TAIWAN APPLIED CRYSTAL CO., LTD. url: https://www.tacrystal.com.
[13] Taiwan Consortium of Emergent Crystalline Materials (TCECM). url: https://tcecmtw.wordpress.com. [14] CMS Collaboration. “Test beam characterization of sensor prototypes for the CMS Barrel MIP Timing Detector”. In: Journal of Instrumentation 16.07 (July 2021), P07023. doi: 10.1088/1748-0221/16/07/P07023. url: https://dx.doi.org/10.1088/1748-0221/16/07/P07023.
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/87168-
dc.description.abstract此論文呈現了與為了高亮度大型強子對撞機而進行的緊湊渺子線圈第二期升級相關的兩個研究。在第一個研究,我們討論了將在第二期升級時取代現有量能器的高粒度量能器的表現。它不僅能提供更好的空間與時間解析度,更是能利用它層狀的構造進行三維的粒子重構。我們呈現了使用高粒度量能器進行濤輕子重構與識別的性能,顯示它在200個對撞事件的積累情況下具有良好的表現。然而為了充分發揮高粒度量能器的潛力,能量校正等數個問題仍需解決。在第二個研究,我們探討了LYSO晶體放光的時間解析度。同樣在緊湊渺子線圈第二期升級時,LYSO晶體將會用於將最小電離粒子時間探測器以提供精確的時間測量。而為了達到如此精確的時間解析度,我們使用了處於蓋格模式下的矽光電倍增元件進行探測。我們呈現了在不同參數設定下所量測到的時間解析度,包括矽光電倍增元件的工作電壓、訊號閾值以及LYSO晶體的大小與摻雜成分。透過我們的設置可以獲得80皮秒的單個LYSO晶體的時間分辨率。zh_TW
dc.description.abstractTwo aspects of studies related to the phase-II upgrade of CMS for the HL-LHC are presented. In the first topic, we discuss the performance of the High Granularity Calorimeter, HGCAL, which will replace pre-shower, ECAL, and HCAL in the end-cap region of CMS. Not only having better resolutions in x, y, and timing measurement, but it also has additional z information and thus can perform a 3D reconstruction. The performance of tau lepton reconstruction and identification with HGCAL are presented and they have good performances under the 200 pile-up situation. Several issues such as energy correction still need to be addressed to achieve the full potential of HGCAL. In the second topic, we study the time resolution of light generated in LYSO crystals. LYSO crystals will be utilized in the MIP Timing detector, MTD, which will also be implemented in the CMS phase-II upgrade for precise time measurement. To reach this time requirement, we make use of Silicon Photon-Multipliers(SiPM), which is a Geiger mode silicon detector. We present the time resolution with several setup parameters, including operation voltage and threshold for SiPMs and different sizes and dopings of LYSO crystals. The time resolution of a single LYSO crystal of 80 picoseconds is obtained with our setup.en
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dc.description.tableofcontents1 Introduction 1
2 The LHC and CMS experiment 2
2.1 Large Hadron Collider . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
2.2 Compact Muon Solenoid . . . . . . . . . . . . . . . . . . . . . . . . . . 2
2.2.1 Magnet System . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
2.2.2 Inner Detector . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
2.2.3 Calorimeter . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
2.2.4 Muon Spectrometer . . . . . . . . . . . . . . . . . . . . . . . . . 4
2.2.5 Particle reconstruction . . . . . . . . . . . . . . . . . . . . . . . 4
2.3 Phase II upgrade . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9
2.3.1 High Granularity Calorimeter . . . . . . . . . . . . . . . . . . . 9
2.3.2 MIP Timing Detector . . . . . . . . . . . . . . . . . . . . . . . . 10
2.3.3 Other upgrades . . . . . . . . . . . . . . . . . . . . . . . . . . . 11
3 Theme I - performance of tau lepton reconstruction and identification in HGCAL 12
3.1 Reconstruction of tau lepton in CMS . . . . . . . . . . . . . . . . . . . 12
3.1.1 Tau reconstruction with CMS . . . . . . . . . . . . . . . . . . . 12
3.2 Identification of tau lepton in CMS . . . . . . . . . . . . . . . . . . . . 14
3.2.1 Discrimination of τh candidates against jets . . . . . . . . . . . 14
3.2.2 Discrimination of τh candidates against electrons . . . . . . . . . 14
3.2.3 Discrimination of τh candidates against muons . . . . . . . . . . 15
3.3 Monte Carlo samples and settings . . . . . . . . . . . . . . . . . . . . . 15
3.4 Reconstruction performance . . . . . . . . . . . . . . . . . . . . . . . . 15
3.4.1 Reconstruction efficiency . . . . . . . . . . . . . . . . . . . . . . 15
3.4.2 Transverse momentum response . . . . . . . . . . . . . . . . . . 16
3.4.3 Reconstructed boson mass . . . . . . . . . . . . . . . . . . . . . 17
3.4.4 Decay mode migration . . . . . . . . . . . . . . . . . . . . . . . 17
3.5 Identification performance . . . . . . . . . . . . . . . . . . . . . . . . . 18
3.5.1 Identification efficiency . . . . . . . . . . . . . . . . . . . . . . . 18
3.5.2 Fake rate . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 18
3.5.3 Identification performance against jet . . . . . . . . . . . . . . . 19
3.5.4 Identification performance against electron . . . . . . . . . . . . 23
3.5.5 Identification performance against muon . . . . . . . . . . . . . 27
3.6 Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 30
4 Theme II - LYSO time resolution measurement with Silicon photo-multipliers 31
4.1 Silicon photomultipliers-LYSO detector . . . . . . . . . . . . . . . . . . 31
4.1.1 Silicon photomultipliers sensor . . . . . . . . . . . . . . . . . . . 31
4.1.2 LYSO crystal . . . . . . . . . . . . . . . . . . . . . . . . . . . . 32
4.2 Experiment setup . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33
4.2.1 Circuit for SiPM and readouts . . . . . . . . . . . . . . . . . . . 34
4.2.2 Operating voltage of SiPM . . . . . . . . . . . . . . . . . . . . . 36
4.2.3 Data Acquisition Systems . . . . . . . . . . . . . . . . . . . . . 37
4.2.4 Data analysis . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37
4.3 Time resolution . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38
4.3.1 Laser calibration . . . . . . . . . . . . . . . . . . . . . . . . . . 38
4.3.2 Coincidence time resolution . . . . . . . . . . . . . . . . . . . . 40
4.4 Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43
5 Conclusion 43
References 43
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dc.language.isoen-
dc.subject緊湊渺子線圈zh_TW
dc.subject濤輕子zh_TW
dc.subject高粒度量能器zh_TW
dc.subject矽光電倍增元件zh_TW
dc.subjectLYSO晶體zh_TW
dc.subjectHGCALen
dc.subjecttau leptonen
dc.subjectSiPMen
dc.subjectCMSen
dc.subjectLYSOen
dc.title緊湊渺子線圈第二期升級研究:濤輕子在高粒度量能器中的重構與辨識及使用矽光電倍增元件量測LYSO之時間解析度zh_TW
dc.titleStudies of CMS Phase II Upgrade: Tau Lepton Reconstruction and Identification in HGCAL and LYSO Time Resolution with SiPMen
dc.typeThesis-
dc.date.schoolyear111-1-
dc.description.degree碩士-
dc.contributor.oralexamcommittee裴思達;陳凱風zh_TW
dc.contributor.oralexamcommitteeStathes Paganis;Kai-Feng Chenen
dc.subject.keyword緊湊渺子線圈,高粒度量能器,濤輕子,矽光電倍增元件,LYSO晶體,zh_TW
dc.subject.keywordCMS,HGCAL,tau lepton,SiPM,LYSO,en
dc.relation.page44-
dc.identifier.doi10.6342/NTU202300425-
dc.rights.note同意授權(全球公開)-
dc.date.accepted2023-02-16-
dc.contributor.author-college理學院-
dc.contributor.author-dept物理學系-
顯示於系所單位:物理學系

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