Study of η(1405)/η(1475) in J / ψ → γ K S 0 K S 0 π 0 $$ J/\psi \to \gamma {K}_S^0{K}_S^0{\pi}^0 $$ decay

Ablikim, M.; Achasov, M.; Adlarson, P.; Albrecht, M.; Aliberti, R.; Amoroso, A.; An, M.; An, Q.; Bai, X.; Bai, Y.; Bakina, O.; Baldini Ferroli, R.; Balossino, I.; Ban, Y.; Batozskaya, V.; Becker, D.; Begzsuren, K.; Berger, N.; Bertani, M.; Bettoni, D.; Bianchi, F.; Bloms, J.; Bortone, A.; Boyko, I.; Briere, R.; Brueggemann, A.; Cai, H.; Cai, X.; Calcaterra, A.; Cao, G.; Cao, N.; Cetin, S.; Chang, J.; Chang, W.; Chelkov, G.; Chen, C.; Chen, Chao; Chen, G.; Chen, H.; Chen, M.; Chen, S.; Chen, S.; Chen, T.; Chen, X.; Chen, X.; Chen, Y.; Chen, Z.; Cheng, W.; Choi, S.; Chu, X.; Cibinetto, G.; Cossio, F.; Cui, J.; Dai, H.; Dai, J.; Dbeyssi, A.; Boer, R.; Dedovich, D.; Deng, Z.; Denig, A.; Denysenko, I.; Destefanis, M.; Mori, F.; Ding, Y.; Dong, J.; Dong, L.; Dong, M.; Dong, X.; Du, S.; Egorov, P.; Fan, Y.; Fang, J.; Fang, S.; Fang, W.; Fang, Y.; Farinelli, R.; Fava, L.; Feldbauer, F.; Felici, G.; Feng, C.; Feng, J.; Fischer, K; Fritsch, M.; Fritzsch, C.; Fu, C.; Gao, H.; Gao, Y.; Gao, Yang; Garbolino, S.; Garzia, I.; Ge, P.; Ge, Z.; Geng, C.; Gersabeck, E.; Gilman, A; Goetzen, K.; Gong, L.; Gong, W.; Gradl, W.; Greco, M.; Gu, L.; Gu, M.; Gu, Y.; Guan, C.; Guo, A.; Guo, L.; Guo, R.; Guo, Y.; Guskov, A.; Han, T.; Han, W.; Hao, X.; Harris, F.; He, K.; He, K.; Heinsius, F.; Heinz, C.; Heng, Y.; Herold, C.; Himmelreich, M.; Hou, G.; Hou, Y.; Hou, Z.; Hu, H.; Hu, J.; Hu, T.; Hu, Y.; Huang, G.; Huang, K.; Huang, L.; Huang, L.; Huang, X.; Huang, Y.; Huang, Z.; Hussain, T.; Hüsken, N; Imoehl, W.; Irshad, M.; Jackson, J.; Jaeger, S.; Janchiv, S.; Jang, E.; Jeong, J.; Ji, Q.; Ji, Q.; Ji, X.; Ji, X.; Ji, Y.; Jia, Z.; Jiang, H.; Jiang, S.; Jiang, X.; Jiang, Y.; Jiang, Yi; Jiao, J.; Jiao, Z.; Jin, S.; Jin, Y.; Jing, M.; Johansson, T.; Kalantar-Nayestanaki, N.; Kang, X.; Kappert, R.; Ke, B.; Keshk, I.; Khoukaz, A.; Kiuchi, R.; Kliemt, R.; Koch, L.; Kolcu, O.; Kopf, B.; Kuemmel, M.; Kuessner, M.; Kupsc, A.; 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, 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, L.; Li, Lei; Li, M.; Li, P.; Li, S.; Li, S.; Li, T.; 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, H.; Liu, H.; Liu, Huanhuan; Liu, Huihui; Liu, J.; Liu, J.; Liu, J.; Liu, K.; Liu, K.; Liu, Ke; Liu, L.; Liu, Lu; Liu, M.; Liu, P.; Liu, Q.; Liu, S.; Liu, T.; Liu, W.; Liu, W.; Liu, X.; Liu, Y.; Liu, Y.; Liu, Z.; Liu, Z.; Lou, X.; Lu, F.; Lu, H.; Lu, J.; Lu, X.; Lu, Y.; Lu, Y.; Lu, Z.; Luo, C.; Luo, M.; Luo, T.; Luo, X.; Lyu, X.; Lyu, Y.; Ma, F.; Ma, H.; Ma, L.; Ma, M.; Ma, Q.; Ma, R.; Ma, R.; Ma, X.; Ma, Y.; Maas, F.; Maggiora, M.; Maldaner, S.; Malde, S.; Malik, Q.; Mangoni, A.; Mao, Y.; Mao, Z.; Marcello, S.; Meng, Z.; 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doi:10.1007/JHEP03(2023)121
Study of η(1405)/η(1475) in $J / ψ \to γ K_{S}^{0} K_{S}^{0} π^{0}$ $$ J/\psi \to \gamma {K}_S^0{K}_S^0{\pi}^0 $$ decay

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) ; M. Albrecht (Bochum Ruhr-University, Bochum, D-44780, Germany) ; R. Aliberti (Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, Mainz, D-55099, Germany) ; et al. - Show all 575 authors
Using a sample of (10.09 ± 0.04) × 109 J/ψ decays collected with the BESIII detector, partial wave analyses of the decay $J / ψ \to γ K_{S}^{0} K_{S}^{0} π^{0}$ $$ J/\psi \to \gamma {K}_S^0{K}_S^0{\pi}^0 $$ are performed within the $K_{S}^{0} K_{S}^{0} π^{0}$ $$ {K}_S^0{K}_S^0{\pi}^0 $$ invariant mass region below 1.6 GeV/c 2. The covariant tensor amplitude method is used in both mass independent and mass dependent approaches. Both analysis approaches exhibit dominant pseudoscalar and axial vector components, and show good consistency for the other individual components. Furthermore, the mass dependent analysis reveals that the $K_{S}^{0} K_{S}^{0} π^{0}$ $$ {K}_S^0{K}_S^0{\pi}^0 $$ invariant mass spectrum for the pseudoscalar component can be well described with two isoscalar resonant states using relativistic Breit-Wigner model, i.e., the η(1405) with a mass of $1391.7 \pm {0.7}_{- 0.3}^{+ 11.3}$ $$ 1391.7\pm {0.7}_{-0.3}^{+11.3} $$ MeV/c 2 and a width of $60.8 \pm {1.2}_{- 12.0}^{+ 5.5}$ $$ 60.8\pm {1.2}_{-12.0}^{+5.5} $$ MeV, and the η(1475) with a mass of $1507.6 \pm {1.6}_{- 32.2}^{+ 15.5}$ $$ 1507.6\pm {1.6}_{-32.2}^{+15.5} $$ MeV/c 2 and a width of $115.8 \pm {2.4}_{- 10.9}^{+ 14.8}$ $$ 115.8\pm {2.4}_{-10.9}^{+14.8} $$ MeV. The first and second uncertainties are statistical and systematic, respectively. Alternate models for the pseudoscalar component are also tested, but the description of the $K_{S}^{0} K_{S}^{0} π^{0}$ $$ {K}_S^0{K}_S^0{\pi}^0 $$ invariant mass spectrum deteriorates significantly.
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  "titles": [
    {
      "source": "Springer", 
      "title": "Study of \u03b7(1405)/\u03b7(1475) in   <math> <mi>J</mi> <mo>/</mo> <mi>\u03c8</mi> <mo>\u2192</mo> <mi>\u03b3</mi> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msup> <mi>\u03c0</mi> <mn>0</mn> </msup> </math>  $$ J/\\psi \\to \\gamma {K}_S^0{K}_S^0{\\pi}^0 $$  decay"
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      "year": 2023, 
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      "journal_issue": "3"
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      "holder": "The Author(s)", 
      "year": "2023"
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  "control_number": "76584", 
  "collaborations": [
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      "value": "The BESIII collaboration"
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  "abstracts": [
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      "source": "Springer", 
      "value": "Using a sample of (10.09 \u00b1 0.04) \u00d7 109 J/\u03c8 decays collected with the BESIII detector, partial wave analyses of the decay   <math> <mi>J</mi> <mo>/</mo> <mi>\u03c8</mi> <mo>\u2192</mo> <mi>\u03b3</mi> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msup> <mi>\u03c0</mi> <mn>0</mn> </msup> </math>  $$ J/\\psi \\to \\gamma {K}_S^0{K}_S^0{\\pi}^0 $$  are performed within the   <math> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msup> <mi>\u03c0</mi> <mn>0</mn> </msup> </math>  $$ {K}_S^0{K}_S^0{\\pi}^0 $$  invariant mass region below 1.6 GeV/c 2. The covariant tensor amplitude method is used in both mass independent and mass dependent approaches. Both analysis approaches exhibit dominant pseudoscalar and axial vector components, and show good consistency for the other individual components. Furthermore, the mass dependent analysis reveals that the   <math> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msup> <mi>\u03c0</mi> <mn>0</mn> </msup> </math>  $$ {K}_S^0{K}_S^0{\\pi}^0 $$  invariant mass spectrum for the pseudoscalar component can be well described with two isoscalar resonant states using relativistic Breit-Wigner model, i.e., the \u03b7(1405) with a mass of   <math> <mn>1391.7</mn> <mo>\u00b1</mo> <msubsup> <mn>0.7</mn> <mrow> <mo>\u2212</mo> <mn>0.3</mn> </mrow> <mrow> <mo>+</mo> <mn>11.3</mn> </mrow> </msubsup> </math>  $$ 1391.7\\pm {0.7}_{-0.3}^{+11.3} $$  MeV/c 2 and a width of   <math> <mn>60.8</mn> <mo>\u00b1</mo> <msubsup> <mn>1.2</mn> <mrow> <mo>\u2212</mo> <mn>12.0</mn> </mrow> <mrow> <mo>+</mo> <mn>5.5</mn> </mrow> </msubsup> </math>  $$ 60.8\\pm {1.2}_{-12.0}^{+5.5} $$  MeV, and the \u03b7(1475) with a mass of   <math> <mn>1507.6</mn> <mo>\u00b1</mo> <msubsup> <mn>1.6</mn> <mrow> <mo>\u2212</mo> <mn>32.2</mn> </mrow> <mrow> <mo>+</mo> <mn>15.5</mn> </mrow> </msubsup> </math>  $$ 1507.6\\pm {1.6}_{-32.2}^{+15.5} $$  MeV/c 2 and a width of   <math> <mn>115.8</mn> <mo>\u00b1</mo> <msubsup> <mn>2.4</mn> <mrow> <mo>\u2212</mo> <mn>10.9</mn> </mrow> <mrow> <mo>+</mo> <mn>14.8</mn> </mrow> </msubsup> </math>  $$ 115.8\\pm {2.4}_{-10.9}^{+14.8} $$  MeV. The first and second uncertainties are statistical and systematic, respectively. Alternate models for the pseudoscalar component are also tested, but the description of the   <math> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msubsup> <mi>K</mi> <mi>S</mi> <mn>0</mn> </msubsup> <msup> <mi>\u03c0</mi> <mn>0</mn> </msup> </math>  $$ {K}_S^0{K}_S^0{\\pi}^0 $$  invariant mass spectrum deteriorates significantly."
    }
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  "imprints": [
    {
      "date": "2023-03-17", 
      "publisher": "Springer"
    }
  ]
}
Published on:: 17 March 2023
Publisher:: Springer
Published in:: Journal of High Energy Physics , Volume 2023 (2023)
Issue 3
Pages 1-31
DOI:: https://doi.org/10.1007/JHEP03(2023)121
arXiv:: 2209.11175
Copyrights:: The Author(s)
Licence:: CC-BY-4.0
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