Search for the decay h c → π 0 J/ψ

Ablikim, M.; Achasov, M.; Adlarson, P.; Ahmed, S.; Albrecht, M.; Aliberti, R.; Amoroso, A.; An, M.; An, Q.; Bai, X.; Bai, Y.; Bakina, O.; Baldini Ferroli, R.; Balossino, I.; Ban, Y.; Begzsuren, K.; Berger, N.; Bertani, M.; Bettoni, D.; Bianchi, F.; Bloms, J.; Bortone, A.; Boyko, I.; Briere, R.; Cai, H.; Cai, X.; Calcaterra, A.; Cao, G.; Cao, N.; Cetin, S.; Chang, J.; Chang, W.; Chelkov, G.; Chen, D.; Chen, G.; Chen, H.; Chen, M.; Chen, S.; Chen, X.; Chen, Y.; Chen, Z.; Cheng, W.; Cibinetto, G.; Cossio, F.; Cui, X.; Dai, H.; Dai, J.; Dai, X.; Dbeyssi, A.; Boer, R.; Dedovich, D.; Deng, Z.; Denig, A.; Denysenko, I.; Destefanis, M.; Mori, F.; Ding, Y.; Dong, C.; Dong, J.; Dong, L.; Dong, M.; Dong, X.; Du, S.; Fan, Y.; Fang, J.; Fang, S.; Fang, Y.; Farinelli, R.; Fava, L.; Feldbauer, F.; Felici, G.; Feng, C.; Feng, J.; Fritsch, M.; Fu, C.; Gao, Y.; Gao, Y.; Gao, Y.; Garzia, I.; Ge, P.; Geng, C.; Gersabeck, E.; Gilman, A.; Goetzen, K.; Gong, L.; Gong, W.; Gradl, W.; Greco, M.; Gu, L.; Gu, M.; Guan, C.; Guo, A.; Guo, A.; Guo, L.; Guo, R.; Guo, Y.; Guskov, A.; Han, T.; Han, W.; Hao, X.; Harris, F.; He, K.; Heinsius, F.; Heinz, C.; Heng, Y.; Herold, C.; Himmelreich, M.; Holtmann, T.; Hou, G.; Hou, Y.; Hou, Z.; Hu, H.; Hu, J.; Hu, T.; Hu, Y.; Huang, G.; Huang, L.; Huang, X.; Huang, Y.; Huang, Z.; Hussain, T.; Hüsken, N.; Ikegami Andersson, W.; Imoehl, W.; Irshad, M.; Jaeger, S.; Janchiv, S.; Ji, Q.; Ji, Q.; Ji, X.; Ji, X.; Ji, Y.; Jiang, H.; Jiang, X.; Jiao, J.; Jiao, Z.; Jin, S.; Jin, Y.; Jing, M.; Johansson, T.; Kalantar-Nayestanaki, N.; Kang, X.; Kappert, R.; Kavatsyuk, M.; Ke, B.; Keshk, I.; Khoukaz, A.; Kiese, P.; Kiuchi, R.; Kliemt, R.; Koch, L.; Kolcu, O.; Kopf, B.; Kuemmel, M.; Kuessner, M.; Kupsc, A.; Kurth, M.; Kühn, W.; Lane, J.; Lange, J.; Larin, P.; Lavania, A.; Lavezzi, L.; Lei, Z.; Leithoff, H.; Lellmann, M.; Lenz, T.; Li, C.; Li, C.; Li, Cheng; Li, D.; Li, F.; Li, G.; Li, H.; Li, H.; Li, H.; Li, H.; Li, H.; Li, J.; Li, J.; Li, J.; Li, Ke; Li, L.; Li, Lei; Li, P.; Li, S.; Li, W.; Li, W.; Li, X.; Li, X.; Li, Xiaoyu; Li, Z.; Liang, H.; Liang, H.; Liang, H.; Liang, Y.; Liang, Y.; Liao, G.; Liao, L.; Libby, J.; Limphirat, A.; Lin, C.; Lin, D.; Lin, T.; Liu, B.; Liu, C.; Liu, D.; Liu, F.; Liu, Fang; Liu, Feng; Liu, G.; Liu, H.; Liu, Huanhuan; Liu, Huihui; Liu, J.; Liu, J.; Liu, J.; Liu, K.; Liu, K.; Liu, Ke; Liu, L.; Liu, M.; Liu, P.; Liu, Q.; Liu, Q.; Liu, S.; Liu, T.; Liu, T.; Liu, W.; Liu, X.; Liu, Y.; Liu, Y.; Liu, Z.; Liu, Z.; Lou, X.; Lu, F.; Lu, H.; Lu, J.; Lu, J.; Lu, X.; Lu, Y.; Lu, Y.; Luo, C.; Luo, M.; Luo, P.; Luo, T.; Luo, X.; Lyu, X.; Ma, F.; Ma, H.; Ma, L.; Ma, M.; Ma, Q.; Ma, R.; Ma, R.; Ma, X.; Ma, X.; Maas, F.; Maggiora, M.; Maldaner, S.; Malde, S.; Malik, Q.; Mangoni, A.; Mao, Y.; Mao, Z.; Marcello, S.; Meng, Z.; Messchendorp, J.; Mezzadri, G.; Min, T.; Mitchell, R.; Mo, X.; Muchnoi, N.; Muramatsu, H.; Nakhoul, S.; Nefedov, Y.; Nerling, F.; Nikolaev, I.; Ning, Z.; Nisar, S.; Olsen, S.; Ouyang, Q.; Pacetti, S.; Pan, X.; Pan, Y.; Pathak, A.; Pathak, A.; Patteri, P.; Pelizaeus, M.; Peng, H.; Peters, K.; Pettersson, J.; Ping, J.; Ping, R.; Pogodin, S.; Poling, R.; Prasad, V.; Qi, H.; Qi, H.; Qi, M.; Qi, T.; Qian, S.; Qian, W.; Qian, Z.; Qiao, C.; Qin, J.; Qin, L.; Qin, X.; Qin, X.; Qin, Z.; Qiu, J.; Qu, S.; Rashid, K.; Ravindran, K.; Redmer, C.; Rivetti, A.; Rodin, V.; Rolo, M.; Rong, G.; Rosner, Ch.; Rump, M.; Sang, H.; Sarantsev, A.; Schelhaas, Y.; Schnier, C.; Schoenning, K.; Scodeggio, M.; Shan, W.; Shan, X.; Shangguan, J.; Shao, M.; Shen, C.; Shen, H.; Shen, X.; Shi, H.; Shi, R.; Shi, X.; Shi, X.; Song, J.; Song, J.; Song, W.; Song, Y.; Sosio, S.; Spataro, S.; Su, K.; Su, P.; Sui, F.; Sun, G.; Sun, H.; Sun, J.; Sun, L.; Sun, S.; Sun, T.; Sun, W.; Sun, X.; Sun, Y.; Sun, Y.; Sun, Z.; Tan, Y.; Tan, Y.; Tang, C.; Tang, G.; Tang, J.; Teng, J.; Thoren, V.; Tian, W.; Tian, Y.; Uman, I.; Wang, B.; Wang, C.; Wang, D.; Wang, H.; Wang, H.; Wang, K.; Wang, L.; Wang, M.; Wang, M.; Wang, Meng; Wang, S.; Wang, W.; Wang, W.; Wang, W.; Wang, X.; Wang, X.; Wang, X.; Wang, Y.; Wang, Y.; Wang, Y.; Wang, Y.; Wang, Y.; Wang, Z.; Wang, Z.; Wang, Ziyi; Wang, Zongyuan; Wei, D.; Weidner, F.; Wen, S.; White, D.; Wiedner, U.; Wilkinson, G.; Wolke, M.; Wollenberg, L.; Wu, J.; Wu, L.; Wu, L.; Wu, X.; Wu, X.; Wu, Z.; Xia, L.; Xiao, H.; Xiao, S.; Xiao, Z.; Xie, X.; Xie, Y.; Xie, Y.; Xing, T.; Xu, C.; Xu, G.; Xu, Q.; Xu, W.; Xu, X.; Xu, Y.; Yan, F.; Yan, L.; Yan, W.; Yan, W.; Yang, H.; Yang, H.; Yang, L.; Yang, S.; Yang, Y.; Yang, Yifan; Yang, Zhi; Ye, M.; Ye, M.; Yin, J.; You, Z.; Yu, B.; Yu, C.; Yu, G.; Yu, J.; Yu, T.; Yuan, C.; Yuan, L.; Yuan, X.; Yuan, Y.; Yuan, Z.; Yue, C.; Zafar, A.; Zeng Zeng, X.; Zeng, Y.; Zhang, A.; Zhang, B.; Zhang, Guangyi; Zhang, H.; Zhang, H.; Zhang, H.; Zhang, H.; Zhang, J.; Zhang, J.; Zhang, J.; Zhang, J.; Zhang, J.; Zhang, Jianyu; Zhang, Jiawei; Zhang, L.; Zhang, L.; Zhang, Lei; Zhang, S.; Zhang, S.; Zhang, Shulei; Zhang, X.; Zhang, X.; Zhang, Y.; Zhang, Y.; Zhang, Y.; Zhang, Yan; Zhang, Yao; Zhang, Z.; Zhao, G.; Zhao, J.; Zhao, J.; Zhao, J.; Zhao, Lei; Zhao, Ling; Zhao, M.; Zhao, Q.; Zhao, S.; Zhao, Y.; Zhao, Y.; Zhao, Z.; Zhemchugov, A.; Zheng, B.; Zheng, J.; Zheng, Y.; Zhong, B.; Zhong, C.; Zhou, L.; Zhou, Q.; Zhou, X.; Zhou, X.; Zhou, X.; Zhou, X.; Zhu, A.; Zhu, J.; Zhu, K.; Zhu, K.; Zhu, S.; Zhu, T.; Zhu, W.; Zhu, W.; Zhu, Y.; Zhu, Z.; Zou, B.; Zou, J.
doi:10.1007/JHEP05(2022)003
Search for the decay h c → π 0 J/ψ

M. Ablikim (Institute of High Energy Physics, Beijing, 100049, People’s Republic of China) ; M. Achasov (G.I. Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk, 630090, Russia; Novosibirsk State University, Novosibirsk, 630090, Russia) ; P. Adlarson (Uppsala University, Uppsala, SE-75120, Sweden) ; S. Ahmed (Helmholtz Institute Mainz, Staudinger Weg 18, Mainz, D-55099, Germany) ; M. Albrecht (Bochum Ruhr-University, Bochum, D-44780, Germany) ; et al. - Show all 515 authors
A search for the decay h c → π 0 J/ψ is performed using a sample of hc produced in the reaction e + e − → π + π − h c . The data samples were collected with the BESIII detector at center-of-mass energies between 4.189 and 4.437 GeV, corresponding to a total integrated luminosity of 11 fb −1. No significant signal is observed. Upper limits on the branching ratio $B$ $$ \mathcal{B} $$ (h c → π 0 J/ψ)/ $B$ $$ \mathcal{B} $$ (h c → γη c → γK + K − π 0) and on the branching fraction $B$ $$ \mathcal{B} $$ (h c → π 0 J/ψ) are determined to be 7.5 × 10 −2 and 4.7 × 10 −4 at 90% confidence level, respectively. The latter is derived from the former using the measured branching fraction of the normalization channel. This is the first determination of the upper limit of the decay h c → π 0 J/ψ.
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  "titles": [
    {
      "source": "Springer", 
      "title": "Search for the decay h  c  \u2192 \u03c0 0 J/\u03c8"
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      "year": 2022, 
      "page_start": "1", 
      "journal_issue": "5"
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      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
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  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2022"
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  "control_number": "69777", 
  "collaborations": [
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      "value": "The BESIII collaboration"
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  "abstracts": [
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      "source": "Springer", 
      "value": "A search for the decay h  c  \u2192 \u03c0 0 J/\u03c8 is performed using a sample of hc produced in the reaction e + e  \u2212  \u2192 \u03c0 + \u03c0  \u2212  h  c . The data samples were collected with the BESIII detector at center-of-mass energies between 4.189 and 4.437 GeV, corresponding to a total integrated luminosity of 11 fb \u22121. No significant signal is observed. Upper limits on the branching ratio   <math> <mi>B</mi> </math>  $$ \\mathcal{B} $$ (h  c  \u2192 \u03c0 0 J/\u03c8)/   <math> <mi>B</mi> </math>  $$ \\mathcal{B} $$ (h  c  \u2192 \u03b3\u03b7  c  \u2192 \u03b3K + K  \u2212  \u03c0 0) and on the branching fraction   <math> <mi>B</mi> </math>  $$ \\mathcal{B} $$ (h  c  \u2192 \u03c0 0 J/\u03c8) are determined to be 7.5 \u00d7 10 \u22122 and 4.7 \u00d7 10 \u22124 at 90% confidence level, respectively. The latter is derived from the former using the measured branching fraction of the normalization channel. This is the first determination of the upper limit of the decay h  c  \u2192 \u03c0 0 J/\u03c8."
    }
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  "imprints": [
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      "date": "2022-05-02", 
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}
Published on:: 02 May 2022
Publisher:: Springer
Published in:: Journal of High Energy Physics , Volume 2022 (2022)
Issue 5
Pages 1-15
DOI:: https://doi.org/10.1007/JHEP05(2022)003
arXiv:: 2111.13915
Copyrights:: The Author(s)
Licence:: CC-BY-4.0
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