Amplitude analysis and branching-fraction measurement of D s + $$ {\mathrm{D}}_{\mathrm{s}}^{+} $$ → π + π 0 η′

Ablikim, M.; Achasov, M.; Adlarson, P.; Ahmed, S.; Albrecht, M.; Aliberti, R.; Amoroso, A.; An, M.; An, Q.; Bai, X.; Bai, Y.; Bakina, O.; 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, 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.; 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.; Gu, S.; Gu, Y.; Guan, C.; Guo, A.; Guo, L.; Guo, R.; Guo, Y.; Guskov, A.; Han, T.; Han, W.; Hao, X.; Harris, F.; He, K.; Heinsius, F.; Heinz, C.; Held, T.; 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.; 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, C.; Li, D.; Li, F.; Li, G.; Li, H.; Li, H.; Li, H.; Li, H.; Li, J.; Li, J.; Li, J.; Li, K.; Li, L.; Li, L.; Li, P.; Li, S.; Li, W.; Li, W.; Li, X.; Li, X.; Li, X.; Li, Z.; Liang, H.; Liang, H.; Liang, H.; Liang, Y.; Liang, Y.; Liao, G.; Liao, L.; Libby, J.; Lin, C.; Liu, B.; Liu, C.; Liu, D.; Liu, F.; Liu, F.; Liu, F.; Liu, H.; Liu, H.; Liu, H.; Liu, H.; Liu, J.; Liu, J.; Liu, J.; Liu, K.; Liu, K.; Liu, L.; Liu, M.; Liu, P.; Liu, Q.; Liu, Q.; Liu, S.; Liu, S.; 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.; Mo, Y.; 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.; Poling, R.; Prasad, V.; Qi, H.; Qi, H.; Qi, K.; Qi, M.; Qi, T.; Qian, S.; Qian, W.; Qian, Z.; Qiao, C.; 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, C.; Rump, M.; Sang, H.; Sarantsev, A.; Schelhaas, Y.; Schnier, C.; Schoenning, K.; Scodeggio, M.; Shan, D.; Shan, W.; Shan, X.; Shangguan, J.; Shao, M.; Shen, C.; Shen, H.; Shen, P.; Shen, X.; Shi, H.; Shi, R.; Shi, X.; Shi, X.; 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, W.; Sun, X.; Sun, Y.; 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, M.; Wang, W.; Wang, W.; Wang, W.; Wang, X.; Wang, X.; Wang, X.; Wang, Y.; Wang, Y.; Wang, Y.; Wang, Y.; Wang, Y.; Wang, Y.; Wang, Z.; Wang, Z.; Wang, Z.; Wang, Z.; 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, Z.; Xia, L.; Xiao, H.; Xiao, S.; Xiao, Z.; Xie, X.; Xie, Y.; Xie, Y.; Xing, T.; Xu, G.; Xu, Q.; Xu, W.; Xu, X.; Xu, Y.; Yan, F.; Yan, L.; Yan, W.; Yan, W.; Yan, X.; Yang, H.; Yang, H.; Yang, L.; Yang, S.; Yang, Y.; Yang, Y.; Yang, Z.; 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, X.; Zeng, Y.; Zhang, A.; Zhang, B.; Zhang, G.; Zhang, H.; Zhang, H.; Zhang, H.; Zhang, H.; Zhang, J.; Zhang, J.; Zhang, J.; Zhang, J.; Zhang, J.; Zhang, J.; Zhang, J.; Zhang, J.; Zhang, L.; Zhang, L.; Zhang, L.; Zhang, S.; Zhang, S.; Zhang, S.; Zhang, X.; Zhang, X.; Zhang, Y.; Zhang, Y.; Zhang, Y.; Zhang, Y.; Zhang, Y.; Zhang, Z.; Zhang, Z.; Zhao, G.; Zhao, J.; Zhao, J.; Zhao, J.; Zhao, L.; Zhao, L.; Zhao, M.; Zhao, Q.; Zhao, S.; Zhao, Y.; Zhao, Y.; Zhao, Z.; Zhemchugov, A.; Zheng, B.; Zheng, J.; Zheng, Y.; 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, X.; Zhu, Y.; Zhu, Z.; Zou, B.; Zou, J.
doi:10.1007/JHEP04(2022)058
Amplitude analysis and branching-fraction measurement of $D_{s}^{+}$ $$ {\mathrm{D}}_{\mathrm{s}}^{+} $$ → π + π 0 η′

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 518 authors
Using data collected with the BESIII detector in e + e − collisions at center-of-mass energies between 4.178 and 4.226 GeV and corresponding to 6.32 fb −1 of integrated luminosity, we report the amplitude analysis and branching-fraction measurement of the $D_{s}^{+}$ $$ {D}_s^{+} $$ → π + π 0 η′ decay. We find that the dominant intermediate process is $D_{s}^{+}$ $$ {D}_s^{+} $$ → ρ + η′ and the significances of other resonant and nonresonant processes are all less than 3σ. The upper limits on the branching fractions of S-wave and P-wave nonresonant components are set to 0.10% and 0.74% at the 90% confidence level, respectively. In addition, the branching fraction of the $D_{s}^{+}$ $$ {D}_s^{+} $$ → π + π 0 η′ decay is measured to be (6.15 ± 0.25(stat.) ± 0.18(syst.))%, which receives significant contribution only from $D_{s}^{+}$ $$ {D}_s^{+} $$ → ρ + η′ according to the amplitude analysis.
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  "titles": [
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      "source": "Springer", 
      "title": "Amplitude analysis and branching-fraction measurement of   <math> <msubsup> <mi>D</mi> <mi>s</mi> <mo>+</mo> </msubsup> </math>  $$ {\\mathrm{D}}_{\\mathrm{s}}^{+} $$  \u2192 \u03c0 + \u03c0 0 \u03b7\u2032"
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      "journal_volume": "2022", 
      "artid": "JHEP04(2022)058", 
      "year": 2022, 
      "page_start": "1", 
      "journal_issue": "4"
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    "date": "2023-03-10T21:32:00.006658", 
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    "submission_number": "b6222fd2bf8a11eda920065bd8dc6b20"
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      "license": "CC-BY-4.0"
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  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2022"
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  "control_number": "69098", 
  "collaborations": [
    {
      "value": "The BESIII collaboration"
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  "abstracts": [
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      "source": "Springer", 
      "value": "Using data collected with the BESIII detector in e + e  \u2212  collisions at center-of-mass energies between 4.178 and 4.226 GeV and corresponding to 6.32 fb \u22121 of integrated luminosity, we report the amplitude analysis and branching-fraction measurement of the   <math> <msubsup> <mi>D</mi> <mi>s</mi> <mo>+</mo> </msubsup> </math>  $$ {D}_s^{+} $$  \u2192 \u03c0 + \u03c0 0 \u03b7\u2032 decay. We find that the dominant intermediate process is   <math> <msubsup> <mi>D</mi> <mi>s</mi> <mo>+</mo> </msubsup> </math>  $$ {D}_s^{+} $$  \u2192 \u03c1 + \u03b7\u2032 and the significances of other resonant and nonresonant processes are all less than 3\u03c3. The upper limits on the branching fractions of S-wave and P-wave nonresonant components are set to 0.10% and 0.74% at the 90% confidence level, respectively. In addition, the branching fraction of the   <math> <msubsup> <mi>D</mi> <mi>s</mi> <mo>+</mo> </msubsup> </math>  $$ {D}_s^{+} $$  \u2192 \u03c0 + \u03c0 0 \u03b7\u2032 decay is measured to be (6.15 \u00b1 0.25(stat.) \u00b1 0.18(syst.))%, which receives significant contribution only from   <math> <msubsup> <mi>D</mi> <mi>s</mi> <mo>+</mo> </msubsup> </math>  $$ {D}_s^{+} $$  \u2192 \u03c1 + \u03b7\u2032 according to the amplitude analysis."
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      "date": "2022-04-08", 
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}
Published on:: 08 April 2022
Publisher:: Springer
Published in:: Journal of High Energy Physics , Volume 2022 (2022)
Issue 4
Pages 1-26
DOI:: https://doi.org/10.1007/JHEP04(2022)058
arXiv:: 2202.04232
Copyrights:: The Author(s)
Licence:: CC-BY-4.0
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