請用此 Handle URI 來引用此文件:
http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/87992
完整後設資料紀錄
DC 欄位 | 值 | 語言 |
---|---|---|
dc.contributor.advisor | 王名儒 | zh_TW |
dc.contributor.advisor | Min-Zu Wang | en |
dc.contributor.author | 蘇鉦皓 | zh_TW |
dc.contributor.author | Jheng-Hao Su | en |
dc.date.accessioned | 2023-08-01T16:16:38Z | - |
dc.date.available | 2023-11-09 | - |
dc.date.copyright | 2023-08-01 | - |
dc.date.issued | 2023 | - |
dc.date.submitted | 2023-07-03 | - |
dc.identifier.citation | [1] The ATLAS Collaboration. Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC. Phys.Lett. B716 (2012) 1-29, 716(1):1–29, Sep 2012.
[2] The CMS Collaboration. Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC. Phys. Lett. B 716 (2012) 30, 716(1):30–61, Sep 2012. [3] M. Yamaga, K. Hanagaki, D. Marlow, S. Vahsen, and K. Abe. Measurement of sin 2ϕ1 in B0 → J/ψ KL Decays. Belle Note 358, 2000. [4] David Griffiths. Intriduction to Elementary Particles. Wiley-VCH, 2008. [5] Mark Thomson. Modern particle physics. Cambridge University Press, 2013. [6] M. Ciuchini, E. Franco, V. Lubicz, G. Martinelli, L. Silvestrini, and C. Tarantino. Power corrections to the CP-violation parameter ε_K. JHEP, 02:181, Feb 2022. [7] R.L. Workman et al. Review of Particle Physics. Prog. Theor. Exp. Phys, 2022. [8] Belle Collaboration. Precise measurement of the CP violation parameter sin 2ϕ1 in B0 → (ccbar)K0 decays. Phys. Rev. Lett. 108, 171802 (2012), 108(17):171802, Apr 2012. [9] Kazunori Akai, Kazuro Furukawa, and Haruyo Koiso. SuperKEKB Collider. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 907:188–199, Nov 2018. [10] T. Abe et al. Belle II Technical Design Report. KEK-REPORT-2010-1, November 2010. [11] I. Adachi, T. E. Browder, P. Križan, S. Tanaka, and Y. Ushiroda. Detectors for extreme luminosity: Belle II. Nucl. Instrum. Meth. A, 907:46–59, 2018. [12] T. Kuhr, C. Pulvermacher, M. Ritter, T. Hauth, and N. Braun. The Belle II Core Software. Comput. Softw. Big Sci. 3 (2019) no.1, 3(1), Nov 2018. [13] David Dossett. Computing and Software at Belle II. EPJ Web Conf., 245:11007, 2020. [14] Thomas Keck. FastBDT: A speed-optimized and cache-friendly implementation of stochastic gradient-boosted decision trees for multivariate classification. Comput. Softw. Big Sci., September 2016. [15] Valeria Fioroni. Study of charmless B → η′ K decays with the Belle II experiment. BELLE2-MTHESIS-2022-005, 2022. [16] Y.-T. Chen, K. Huang, Y.-R. Lin, J.-G. Shiu, and M.-Z. Wang. Particle Indentication of Anti-neutron. BELLE2-NOTE-TE-2020-016, 2020. [17] Claudia Cecchi, Guglielmo De Nardo, Elisa Manoni, and Mario Merola. B counting measurement in ”Moriond 2022/ICHEP 2022” Belle II dataset. BELLE2-NOTE-PH-2022-007, 2022. [18] Belle II Collaboration. Rediscovery of B0 → J/ψ K0L at Belle II. BELLE2-CONFPH-2021-009, June 2021. [19] A. Tchouvikov, K. Korotushenko, D. Marlow, and S. Vahsen. Using e+e− → γϕ decay followed by ϕ → KS KL for KL calibration. Belle Note 580, 2002. | - |
dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/87992 | - |
dc.description.abstract | 我們可以透過從ECL束或KLM束所重建的K0L粒子列表來研究K0L介子。粒子識別(PID)可以幫助我們將K0L從其它粒子,如光子、中子、反中子,和其他電中性粒子區分開來。本論文使用Belle II實驗中ECL的資訊並描述識別K0L粒子之建立、方法、表現及比較。
在這篇論文中,我們使用快速提升決策樹(FastBDT)以獲得訓練過後的多變量分析方法。此方法可以將訊號(K0L)以及背景(K0L以外的所有電中性粒子)。我們呈現重建B0 → J/ψ K0L衰變的初步結果,其中J/ψ會衰變成μ+μ−,而K0L介子是從ECL裡的中性強子束重建而來。在Belle II實驗中使用蒙地卡羅方法單純產生訊號,我們可以從100萬個事件裡得到25%的效率。使用蒙地卡羅方法生成各種粒子時,我們可以從100/fb的光度獲得681±71個訊號事件。此外,我們也使用Belle II實驗在SuperKEKB的非對稱能量e+e−對撞機所收集到光度189.049/fb的數據。在J/ψ → μ+μ−的情況下,我們總共量測到1031±95個訊號事件。我們也比較了上述的結果與從KLM裡的K0L介子重建B0 → J/ψ K0L衰變的結果。透過在訊號生成與真實數據中比較ECL和KLM在全範圍以及訊號範圍的結果,我們發現ECL和KLM並沒有太大的重複性。因此本論文提供了K0L識別的另一個方法。 | zh_TW |
dc.description.abstract | We can study K0L through K0L particle list reconstructed from ECL cluster or KLM cluster. Particle identification (PID) can help separate K0L from other particles, like γ, neutron, anti-neutron and other neutral particles. This thesis shows the establishment, method, performance and the comparison of K0L particle identification by using only ECL information in Belle II experiment.
In this thesis, we use Fast Boosted Decision Tree (FastBDT) to get a trained multivariate analysis (MVA) method which can separate signal (K0L) and background (neutral particles excluding K0L). We present the results on the reconstruction of the B0 → J/ψ K0L decay, where J/ψ → μ+μ−. K0L mesons are reconstructed from the hadronic neutral clusters in the Electromagnetic Calorimeter (ECL). Using signal Monte Carlo (MC) with one millon events in Belle II, we have about 25% efficiency. In generic MC corresponding to a luminosity of 100/fb, we get 681 ± 71 candidates. Moreover, we use the Belle II experiment dataset corresponding to a luminosity of 189.049/fb collected in the asymmetric energy e+e− collider at SuperKEKB. We measure 1031±95 candidates with J/ψ → μ+μ− in total. We also compare the results above with the reconstruction of the B0 → J/ψ K0L decay, while K0L mesons are reconstructed from the hadronic neutral clusters in K0L and muons (KLM) subdetector. By the comparison of the result in ECL and KLM in whole region and signal region with signal MC and Data, we notice that the overlap of ECL and KLM is not large. This provides another way for K0L identification. | en |
dc.description.provenance | Submitted by admin ntu (admin@lib.ntu.edu.tw) on 2023-08-01T16:16:38Z No. of bitstreams: 0 | en |
dc.description.provenance | Made available in DSpace on 2023-08-01T16:16:38Z (GMT). No. of bitstreams: 0 | en |
dc.description.tableofcontents | Acknowledgements . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . iii
摘要. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . iv Abstract . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . v Contents . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ix List of Figures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . xi List of Tables . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . xii 1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1 2 The Standard Model and Belle II . . . . . . . . . . . . . . . . . . . . . . . 3 2.1 Standard Model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3 2.2 CP-violation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5 2.3 SuperKEKB . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9 2.4 Belle II Detector . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10 2.4.1 Vertex detector (VXD) . . . . . . . . . . . . . . . . . . . . . . . 11 2.4.2 Central Drift Chamber (CDC) . . . . . . . . . . . . . . . . . . . 13 2.4.3 Particle identification (PID) system . . . . . . . . . . . . . . . . 14 2.4.4 Electromagnetic Calorimeter (ECL) . . . . . . . . . . . . . . . . 16 2.4.5 K0L - Muon Detector (KLM) . . . . . . . . . . . . . . . . . . . . 18 2.4.6 Detector Solenoid and Iron Structure . . . . . . . . . . . . . . . 20 2.4.7 Trigger system . . . . . . . . . . . . . . . . . . . . . . . . . . . 20 2.4.8 Data Acquisition (DAQ) System . . . . . . . . . . . . . . . . . . 21 3 MVA Method . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 22 3.1 Belle II Analysis Software Framework . . . . . . . . . . . . . . . . . . . 22 3.2 FastBDT . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 22 3.3 Training . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 24 3.3.1 Training Method . . . . . . . . . . . . . . . . . . . . . . . . . . 24 3.3.2 Samples . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 24 3.3.3 Training Variables . . . . . . . . . . . . . . . . . . . . . . . . . 25 3.4 Training Results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 31 4 The B0 → J/ψ K0L Decay with ECL . . . . . . . . . . . . . . . . . . . . . 34 4.1 Event Selection . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 34 4.1.1 J/ψ selection . . . . . . . . . . . . . . . . . . . . . . . . . . . . 34 4.1.2 K0L selection . . . . . . . . . . . . . . . . . . . . . . . . . . . . 36 4.1.3 B0 best candidate . . . . . . . . . . . . . . . . . . . . . . . . . . 37 4.2 B0 mass constraint . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37 4.3 The results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38 4.3.1 B0 → J/ψ K0L decay in signal MC . . . . . . . . . . . . . . . . . 38 4.3.2 B0 → J/ψ K0L decay in generic MC . . . . . . . . . . . . . . . . 39 4.3.3 The validation . . . . . . . . . . . . . . . . . . . . . . . . . . . 40 4.3.4 B0 → J/ψ K0L decay in Data . . . . . . . . . . . . . . . . . . . . 40 5 The B0 → J/ψ K0L Decay with KLM and Comparison . . . . . . . . . . . 42 5.1 Event Selection . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 42 5.1.1 J/ψ selection . . . . . . . . . . . . . . . . . . . . . . . . . . . . 42 5.1.2 K0L selection . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43 5.1.3 B0 best candidate . . . . . . . . . . . . . . . . . . . . . . . . . . 45 5.2 The results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45 5.2.1 B0 → J/ψ K0L decay in signal MC . . . . . . . . . . . . . . . . . 45 5.2.2 B0 → J/ψ K0L decay in generic MC . . . . . . . . . . . . . . . . 46 5.2.3 The validation . . . . . . . . . . . . . . . . . . . . . . . . . . . 46 5.2.4 B0 → J/ψ K0L decay in Data . . . . . . . . . . . . . . . . . . . . 47 5.3 Comparison . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 48 6 Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 50 References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51 A Appendix The MVA distribution of the different training results applying on the test sample . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 53 | - |
dc.language.iso | en | - |
dc.title | 在Belle II實驗中用ECL資訊辨別K0L介子 | zh_TW |
dc.title | The study of K0L Identification with ECL Information at Belle II experiment | en |
dc.type | Thesis | - |
dc.date.schoolyear | 111-2 | - |
dc.description.degree | 碩士 | - |
dc.contributor.oralexamcommittee | 張敏娟;張寶棣;徐靜戈 | zh_TW |
dc.contributor.oralexamcommittee | Ming-Chuan Chang;Pao-Ti Chang;Jing-Ge Shiu | en |
dc.subject.keyword | Belle II,K0L 介子,識別,ECL,FastBDT, | zh_TW |
dc.subject.keyword | Belle II,K0L,identification,ECL,FastBDT, | en |
dc.relation.page | 54 | - |
dc.identifier.doi | 10.6342/NTU202301289 | - |
dc.rights.note | 同意授權(限校園內公開) | - |
dc.date.accepted | 2023-07-05 | - |
dc.contributor.author-college | 理學院 | - |
dc.contributor.author-dept | 應用物理研究所 | - |
顯示於系所單位: | 應用物理研究所 |
文件中的檔案:
檔案 | 大小 | 格式 | |
---|---|---|---|
ntu-111-2.pdf 目前未授權公開取用 | 7.34 MB | Adobe PDF | 檢視/開啟 |
系統中的文件,除了特別指名其著作權條款之外,均受到著作權保護,並且保留所有的權利。