Measurement of e+e−→ηJ/ψ cross section from s=3.808 GeV to 4.951 GeV

Ablikim, M.; Achasov, M. N.; Adlarson, P.; Ai, X. C.; Aliberti, R.; Amoroso, A.; An, M. R.; An, Q.; Bai, Y.; Bakina, O.; Balossino, I.; Ban, Y.; Bao, H.R.; Batozskaya, V.; Begzsuren, K.; Berger, N.; Berlowski, M.; Bertani, M.; Bettoni, D.; Bianchi, F.; Bianco, E.; Bortone, A.; Boyko, I.; Briere, R. A.; Brueggemann, A.; Cai, H.; Cai, X.; Calcaterra, A.; Cao, G. F.; Cao, N.; Cetin, S. A.; Chang, J. F.; Chang, T. T.; Chang, W. L.; Che, G. R.; Chelkov, G.; Chen, C.; Chen, Chao; Chen, G.; Chen, H. S.; Chen, M. L.; Chen, S. J.; Chen, S. L.; Chen, S. M.; Chen, T.; Chen, X. R.; Chen, X. T.; Chen, Y. B.; Chen, Y. Q.; Chen, Z. J.; Choi, S. K.; Chu, X.; Cibinetto, G.; Coen, S. C.; Cossio, F.; Cui, J. J.; Dai, H. L.; Dai, J. P.; Dbeyssi, A.; de Boer, R. E.; Dedovich, D.; Deng, Z. Y.; Denig, A.; Denysenko, I.; Destefanis, M.; De Mori, F.; Ding, B.; Ding, X. X.; Ding, Y.; Ding, Y.; Dong, J.; Dong, L. Y.; Dong, M. Y.; Dong, X.; Du, M. C.; Du, S. X.; Duan, Z. H.; Egorov, P.; Fan, Y. H.; Fang, J.; Fang, S. S.; Fang, W. X.; Fang, Y.; Fang, Y. Q.; Farinelli, R.; Fava, L.; Feldbauer, F.; Felici, G.; Feng, C. Q.; Feng, J. H.; Feng, Y. T.; Fischer, K.; Fritsch, M.; Fu, C. D.; Fu, J. L.; Fu, Y. W.; Gao, H.; Gao, Y. N.; Gao, Yang; Garbolino, S.; Garzia, I.; Ge, P. T.; Ge, Z. W.; Geng, C.; Gersabeck, E. M.; Gilman, A.; Goetzen, K.; Gong, L.; Gong, W. X.; Gradl, W.; Gramigna, S.; Greco, M.; Gu, M. H.; Gu, Y. T.; Guan, C. Y.; Guan, Z. L.; Guo, A. Q.; Guo, L. B.; Guo, M. J.; Guo, R. P.; Guo, Y. P.; Guskov, A.; Gutierrez, J.; Han, T. T.; Han, W. Y.; Hao, X. Q.; Harris, F. A.; He, K. K.; He, K. L.; Heinsius, F. H. H.; Heinz, C. H.; Heng, Y. K.; Herold, C.; Holtmann, T.; Hong, P. C.; Hou, G. Y.; Hou, X. T.; Hou, Y. R.; Hou, Z. L.; Hu, B. Y.; Hu, H. M.; Hu, J. F.; Hu, T.; Hu, Y.; Huang, G. S.; Huang, K. X.; Huang, L. Q.; Huang, X. T.; Huang, Y. P.; Hussain, T.; Hüsken, N.; in der Wiesche, N.; Irshad, M.; Jackson, J.; Jaeger, S.; Janchiv, S.; Jeong, J. H.; Ji, Q.; Ji, Q. P.; Ji, X. B.; Ji, X. L.; Ji, Y. Y.; Jia, X. Q.; Jia, Z. K.; Jiang, H. J.; Jiang, P. C.; Jiang, S. S.; Jiang, T. J.; Jiang, X. S.; Jiang, Y.; Jiao, J. B.; Jiao, Z.; Jin, S.; Jin, Y.; Jing, M. Q.; Jing, X. M.; Johansson, T.; K., X.; Kabana, S.; Kalantar-Nayestanaki, N.; Kang, X. L.; Kang, X. S.; Kavatsyuk, M.; Ke, B. C.; Khachatryan, V.; Khoukaz, A.; Kiuchi, R.; Kliemt, R.; Kolcu, O. B.; Kopf, B.; Kuessner, M.; Kupsc, A.; Kühn, W.; Lane, J. J.; Larin, P.; Lavania, A.; Lavezzi, L.; Lei, T. T.; Lei, Z. H.; Leithoff, H.; Lellmann, M.; Lenz, T.; Li, C.; Li, C.; Li, C. H.; Li, Cheng; Li, D. M.; Li, F.; Li, G.; Li, H.; Li, H. B.; Li, H. J.; Li, H. N.; Li, Hui; Li, J. R.; Li, J. S.; Li, J. W.; Li, Ke; Li, L. J.; Li, L. K.; Li, Lei; Li, M. H.; Li, P. R.; Li, Q. X.; Li, S. X.; Li, T.; Li, W. D.; Li, W. G.; Li, X. H.; Li, X. L.; Li, Xiaoyu; Li, Y. G.; Li, Z. J.; Li, Z. X.; Liang, C.; Liang, H.; Liang, H.; Liang, Y. F.; Liang, Y. T.; Liao, G. R.; Liao, L. Z.; Liao, Y. P.; Libby, J.; Limphirat, A.; Lin, D. X.; Lin, T.; Liu, B. J.; Liu, B. X.; 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Pan, X.; Pan, Y.; Pathak, A.; Patteri, P.; Pei, Y. P.; Pelizaeus, M.; Peng, H. P.; Peng, Y. Y.; Peters, K.; Ping, J. L.; Ping, R. G.; Plura, S.; Prasad, V.; Qi, F. Z.; Qi, H.; Qi, H. R.; Qi, M.; Qi, T. Y.; Qian, S.; Qian, W. B.; Qiao, C. F.; Qin, J. J.; Qin, L. Q.; Qin, X. S.; Qin, Z. H.; Qiu, J. F.; Qu, S. Q.; Redmer, C. F.; Ren, K. J.; Rivetti, A.; Rolo, M.; Rong, G.; Rosner, Ch.; Ruan, S. N.; Salone, N.; Sarantsev, A.; Schelhaas, Y.; Schoenning, K.; Scodeggio, M.; Shan, K. Y.; Shan, W.; Shan, X. Y.; Shangguan, J. F.; Shao, L. G.; Shao, M.; Shen, C. P.; Shen, H. F.; Shen, W. H.; Shen, X. Y.; Shi, B. A.; Shi, H. C.; Shi, J. L.; Shi, J. Y.; Shi, Q. Q.; Shi, R. S.; Shi, X.; Song, J. J.; Song, T. Z.; Song, W. M.; Song, Y. J.; Song, Y. X.; Sosio, S.; Spataro, S.; Stieler, F.; Su, Y. J.; Sun, G. B.; Sun, G. X.; Sun, H.; Sun, H. K.; Sun, J. F.; Sun, K.; Sun, L.; Sun, S. S.; Sun, T.; Sun, W. Y.; Sun, Y.; Sun, Y. J.; Sun, Y. Z.; Sun, Z. T.; Tan, Y. X.; Tang, C. J.; Tang, G. Y.; Tang, J.; Tang, Y. A.; 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Zhang, Yan; Zhang, Yao; Zhang, Z. D.; Zhang, Z. H.; Zhang, Z. L.; Zhang, Z. Y.; Zhang, Z. Y.; Zhao, G.; Zhao, J. Y.; Zhao, J. Z.; Zhao, Lei; Zhao, Ling; Zhao, M. G.; Zhao, R. P.; Zhao, S. J.; Zhao, Y. B.; Zhao, Y. X.; Zhao, Z. G.; Zhemchugov, A.; Zheng, B.; Zheng, J. P.; Zheng, W. J.; Zheng, Y. H.; Zhong, B.; Zhong, X.; Zhou, H.; Zhou, L. P.; Zhou, X.; Zhou, X. K.; Zhou, X. R.; Zhou, X. Y.; Zhou, Y. Z.; Zhu, J.; Zhu, K.; Zhu, K. J.; Zhu, L.; Zhu, L. X.; Zhu, S. H.; Zhu, S. Q.; Zhu, T. J.; Zhu, W. J.; Zhu, Y. C.; Zhu, Z. A.; Zou, J. H.; Zu, J.
doi:10.1103/PhysRevD.109.092012
Measurement of $e^{+} e^{-} \to η J / ψ$ cross section from $\sqrt{s} = 3.808 GeV$ to 4.951 GeV

M. Ablikim (Institute of High Energy Physics, Beijing 100049, People’s Republic of China) ; M. N. Achasov (Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russia) ; P. Adlarson (Uppsala University, Box 516, SE-75120 Uppsala, Sweden) ; X. C. Ai (Zhengzhou University, Zhengzhou 450001, People’s Republic of China) ; R. Aliberti (Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany) ; et al. - Show all 632 authors
Using data samples with an integrated luminosity of $22.42 {fb}^{- 1}$ collected by the BESIII detector operating at the BEPCII storage ring, we measure the cross sections of the $e^{+} e^{-} \to η J / ψ$ process at center-of-mass energies from 3.808 to 4.951 GeV. Three structures are observed in the line shape of the measured cross sections. A maximum-likelihood fit with $ψ (4040)$ , two additional resonances, and a nonresonant component are performed. The mass and width of the first additional state are $(4219.7 \pm 2.5 \pm 4.5) MeV / c^{2}$ and $(80.7 \pm 4.4 \pm 1.4) MeV$ , respectively, consistent with the $ψ (4230)$ . For the second state, the mass and width are $(4386 \pm 13 \pm 17) MeV / c^{2}$ and $(177 \pm 32 \pm 13) MeV$ , respectively, consistent with the $ψ (4360)$ . The first uncertainties are statistical, and the second ones are systematic. The statistical significance of $ψ (4040)$ is $8.0 σ$ and those for $ψ (4230)$ and $ψ (4360)$ are more than $10.0 σ$ .
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      "affiliations": [
        {
          "country": "China", 
          "value": "Institute of High Energy Physics, Beijing 100049, People\u2019s Republic of China"
        }, 
        {
          "country": "China", 
          "value": "University of Chinese Academy of Sciences, Beijing 100049, People\u2019s Republic of China"
        }
      ], 
      "surname": "Zhu", 
      "given_names": "Z.\u2009A.", 
      "full_name": "Zhu, Z.\u2009A."
    }, 
    {
      "raw_name": "J.\u2009H. Zou", 
      "affiliations": [
        {
          "country": "China", 
          "value": "Institute of High Energy Physics, Beijing 100049, People\u2019s Republic of China"
        }
      ], 
      "surname": "Zou", 
      "given_names": "J.\u2009H.", 
      "full_name": "Zou, J.\u2009H."
    }, 
    {
      "raw_name": "J. Zu", 
      "affiliations": [
        {
          "country": "China", 
          "value": "State Key Laboratory of Particle Detection and Electronics, Beijing 100049, Hefei 230026, People\u2019s Republic of China"
        }, 
        {
          "country": "China", 
          "value": "University of Science and Technology of China, Hefei 230026, People\u2019s Republic of China"
        }
      ], 
      "surname": "Zu", 
      "given_names": "J.", 
      "full_name": "Zu, J."
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "Measurement of <math><msup><mi>e</mi><mo>+</mo></msup><msup><mi>e</mi><mo>\u2212</mo></msup><mo>\u2192</mo><mi>\u03b7</mi><mi>J</mi><mo>/</mo><mi>\u03c8</mi></math> cross section from <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>3.808</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi></math> to 4.951 GeV"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevD.109.092012"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "109", 
      "journal_title": "Physical Review D", 
      "material": "article", 
      "journal_issue": "9", 
      "year": 2024
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2024-05-30T00:30:11.427898", 
    "source": "APS", 
    "method": "APS", 
    "submission_number": "bfb514741e1b11efbefa56ef197c8653"
  }, 
  "page_nr": [
    16
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2024"
    }
  ], 
  "control_number": "85888", 
  "collaborations": [
    {
      "value": "BESIII Collaboration"
    }
  ], 
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  "record_creation_date": "2024-05-29T14:30:05.547108", 
  "collections": [
    {
      "primary": "HEP"
    }, 
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      "primary": "Citeable"
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    {
      "primary": "Published"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ex"
      ], 
      "value": "2310.03361"
    }
  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "Using data samples with an integrated luminosity of <math><mn>22.42</mn><mtext> </mtext><mtext> </mtext><msup><mi>fb</mi><mrow><mo>\u2212</mo><mn>1</mn></mrow></msup></math> collected by the BESIII detector operating at the BEPCII storage ring, we measure the cross sections of the <math><msup><mi>e</mi><mo>+</mo></msup><msup><mi>e</mi><mo>\u2212</mo></msup><mo>\u2192</mo><mi>\u03b7</mi><mi>J</mi><mo>/</mo><mi>\u03c8</mi></math> process at center-of-mass energies from 3.808 to 4.951 GeV. Three structures are observed in the line shape of the measured cross sections. A maximum-likelihood fit with <math><mi>\u03c8</mi><mo>(</mo><mn>4040</mn><mo>)</mo></math>, two additional resonances, and a nonresonant component are performed. The mass and width of the first additional state are <math><mo>(</mo><mn>4219.7</mn><mo>\u00b1</mo><mn>2.5</mn><mo>\u00b1</mo><mn>4.5</mn><mo>)</mo><mtext> </mtext><mtext> </mtext><mi>MeV</mi><mo>/</mo><msup><mi>c</mi><mn>2</mn></msup></math> and <math><mo>(</mo><mn>80.7</mn><mo>\u00b1</mo><mn>4.4</mn><mo>\u00b1</mo><mn>1.4</mn><mo>)</mo><mtext> </mtext><mtext> </mtext><mi>MeV</mi></math>, respectively, consistent with the <math><mi>\u03c8</mi><mo>(</mo><mn>4230</mn><mo>)</mo></math>. For the second state, the mass and width are <math><mo>(</mo><mn>4386</mn><mo>\u00b1</mo><mn>13</mn><mo>\u00b1</mo><mn>17</mn><mo>)</mo><mtext> </mtext><mtext> </mtext><mi>MeV</mi><mo>/</mo><msup><mi>c</mi><mn>2</mn></msup></math> and <math><mo>(</mo><mn>177</mn><mo>\u00b1</mo><mn>32</mn><mo>\u00b1</mo><mn>13</mn><mo>)</mo><mtext> </mtext><mtext> </mtext><mi>MeV</mi></math>, respectively, consistent with the <math><mi>\u03c8</mi><mo>(</mo><mn>4360</mn><mo>)</mo></math>. The first uncertainties are statistical, and the second ones are systematic. The statistical significance of <math><mi>\u03c8</mi><mo>(</mo><mn>4040</mn><mo>)</mo></math> is <math><mn>8.0</mn><mi>\u03c3</mi></math> and those for <math><mi>\u03c8</mi><mo>(</mo><mn>4230</mn><mo>)</mo></math> and <math><mi>\u03c8</mi><mo>(</mo><mn>4360</mn><mo>)</mo></math> are more than <math><mn>10.0</mn><mi>\u03c3</mi></math>."
    }
  ], 
  "imprints": [
    {
      "date": "2024-05-29", 
      "publisher": "APS"
    }
  ]
}
Published on:: 29 May 2024
Publisher:: APS
Published in:: Physical Review D , Volume 109 (2024)
Issue 9
DOI:: https://doi.org/10.1103/PhysRevD.109.092012
arXiv:: 2310.03361
Copyrights:: Published by the American Physical Society
Licence:: CC-BY-4.0
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