Search for K L Rare Decay K L → π 0 ν ν ̄ and K L → π 0 X(X → invisible) in KOTO Experiment

碩士 === 國立臺灣大學 === 物理學研究所 === 105 === A search of a direct CP-violating decay K L → π 0 ν ν ̄ is performedin KOTO experiment, which was launched in Japan Proton AcceleratorComplex (J-Parc). K L → π 0 ν ν ̄ is highly suppressed in the Standard Model (SM), and the branch ratio Br(K L → π 0 ν ν ̄ ) =...

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Main Authors: Shih-Hsuan Chen, 陳世軒
Other Authors: Yee Bob Hsiung
Format: Others
Language:en_US
Published: 2017
Online Access:http://ndltd.ncl.edu.tw/handle/8q6x8y
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spelling ndltd-TW-105NTU051980442019-05-15T23:39:39Z http://ndltd.ncl.edu.tw/handle/8q6x8y Search for K L Rare Decay K L → π 0 ν ν ̄ and K L → π 0 X(X → invisible) in KOTO Experiment 在 KOTO 實驗中尋找長生命期中性 K 介子之稀有衰變K L → π 0 ν ν ̄ 以及 K L → π 0 X(X 至不可見粒子 ) Shih-Hsuan Chen 陳世軒 碩士 國立臺灣大學 物理學研究所 105 A search of a direct CP-violating decay K L → π 0 ν ν ̄ is performedin KOTO experiment, which was launched in Japan Proton AcceleratorComplex (J-Parc). K L → π 0 ν ν ̄ is highly suppressed in the Standard Model (SM), and the branch ratio Br(K L → π 0 ν ν ̄ ) = (3.00 ± 0.30) ×10 −11 is given by the SM prediction. Due to its theoretically cleanness, the measurement of K L → π 0 ν ν ̄ branching ratio provide a direct measurement of η in CKM matrix, as well as a good probe to the New Physics. This thesis performs an analysis with data collected in 2015, in which the statistics of data is about 20 times larger than that taken in May 2013. There are 9 periods with different intensity of K L beam during the 4-months data taking in 2015. The analysis of K L flux has been done for each periods using 3 normalization modes: K L → 3π 0 , K L → 2π 0 , and K L → γγ, and the results are consistent with each other. Using the blind analysis method, a search for K L → π 0 ν ν ̄ , which consists of estimation of systematic uncertainty, background study, and normalization, is then performed based on 2015 data. As a preliminary result, the single event sensitivity (S.E.S.) is obtained as S.E.S. = (1.27 ± 0.01 stat ± 0.1 sys ) × 10 −9 . The expected number of background in the signal region is 1.32±0.33. In addition, for K L → π 0 X, (X → invisible) search, X mass is calculated by means of invariant mass of ν ν ̄ in K L → π 0 ν ν ̄ MC simulation, and S.E.S. for M X = M π 0 is obtained as 0.99 × 10 −9 . Yee Bob Hsiung 熊怡 2017 學位論文 ; thesis 137 en_US
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description 碩士 === 國立臺灣大學 === 物理學研究所 === 105 === A search of a direct CP-violating decay K L → π 0 ν ν ̄ is performedin KOTO experiment, which was launched in Japan Proton AcceleratorComplex (J-Parc). K L → π 0 ν ν ̄ is highly suppressed in the Standard Model (SM), and the branch ratio Br(K L → π 0 ν ν ̄ ) = (3.00 ± 0.30) ×10 −11 is given by the SM prediction. Due to its theoretically cleanness, the measurement of K L → π 0 ν ν ̄ branching ratio provide a direct measurement of η in CKM matrix, as well as a good probe to the New Physics. This thesis performs an analysis with data collected in 2015, in which the statistics of data is about 20 times larger than that taken in May 2013. There are 9 periods with different intensity of K L beam during the 4-months data taking in 2015. The analysis of K L flux has been done for each periods using 3 normalization modes: K L → 3π 0 , K L → 2π 0 , and K L → γγ, and the results are consistent with each other. Using the blind analysis method, a search for K L → π 0 ν ν ̄ , which consists of estimation of systematic uncertainty, background study, and normalization, is then performed based on 2015 data. As a preliminary result, the single event sensitivity (S.E.S.) is obtained as S.E.S. = (1.27 ± 0.01 stat ± 0.1 sys ) × 10 −9 . The expected number of background in the signal region is 1.32±0.33. In addition, for K L → π 0 X, (X → invisible) search, X mass is calculated by means of invariant mass of ν ν ̄ in K L → π 0 ν ν ̄ MC simulation, and S.E.S. for M X = M π 0 is obtained as 0.99 × 10 −9 .
author2 Yee Bob Hsiung
author_facet Yee Bob Hsiung
Shih-Hsuan Chen
陳世軒
author Shih-Hsuan Chen
陳世軒
spellingShingle Shih-Hsuan Chen
陳世軒
Search for K L Rare Decay K L → π 0 ν ν ̄ and K L → π 0 X(X → invisible) in KOTO Experiment
author_sort Shih-Hsuan Chen
title Search for K L Rare Decay K L → π 0 ν ν ̄ and K L → π 0 X(X → invisible) in KOTO Experiment
title_short Search for K L Rare Decay K L → π 0 ν ν ̄ and K L → π 0 X(X → invisible) in KOTO Experiment
title_full Search for K L Rare Decay K L → π 0 ν ν ̄ and K L → π 0 X(X → invisible) in KOTO Experiment
title_fullStr Search for K L Rare Decay K L → π 0 ν ν ̄ and K L → π 0 X(X → invisible) in KOTO Experiment
title_full_unstemmed Search for K L Rare Decay K L → π 0 ν ν ̄ and K L → π 0 X(X → invisible) in KOTO Experiment
title_sort search for k l rare decay k l → π 0 ν ν ̄ and k l → π 0 x(x → invisible) in koto experiment
publishDate 2017
url http://ndltd.ncl.edu.tw/handle/8q6x8y
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