<p>Using the data samples of 102 million Υ(1<i>S</i>) and 158 million Υ(2<i>S</i>) events collected by the Belle detector, we search for a pentaquark state in the <i>pJ/ψ</i> final state from Υ(1<i>,</i> 2<i>S</i>) inclusive decays. Here, the charge-conjugate <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27128_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{p }J/\psi \)</EquationSource> </InlineEquation> is included. We observe clear <i>pJ/ψ</i> production in Υ(1<i>,</i> 2<i>S</i>) decays and measure the branching fractions to be <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27128_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="499" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{B}[\Upsilon (1S)\to pJ/\psi +anything]=[8.1\pm 0.6(stat.)\pm 0.5(syst.)]\times {10}^{-5}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27128_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="499" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{B}[\Upsilon (2S)\to pJ/\psi +anything]=[4.3\pm 0.5(stat.)\pm 0.4(syst.)]\times {10}^{-5}\)</EquationSource> </InlineEquation>. We also measure the cross section of inclusive <i>pJ/ψ</i> production in <i>e</i><sup>+</sup><i>e</i><sup><i>−</i></sup> annihilation to be <i>σ</i>(<i>e</i><sup>+</sup><i>e</i><sup><i>−</i></sup> → <i>pJ/ψ</i> + <i>anything</i>) = [108 ± 11(<i>stat.</i>) ± 6(<i>syst.</i>)] fb at <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27128_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="86" /> </InlineMediaObject> <EquationSource Format="TEX">\(\sqrt{s}=10.52\)</EquationSource> </InlineEquation> GeV using an 89<i>.</i>5 fb<sup><i>−</i>1</sup> continuum data sample. There is no significant <i>P</i><sub><i>c</i></sub>(4312)<sup>+</sup>, <i>P</i><sub><i>c</i></sub>(4440)<sup>+</sup> or <i>P</i><sub><i>c</i></sub>(4457)<sup>+</sup> signal found in the <i>pJ/ψ</i> final states in Υ(1<i>,</i> 2<i>S</i>) inclusive decays. We determine the upper limits of <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27128_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="352" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{B}\left[\Upsilon \left({1},{2}S\right)\to {P}_{c}^{+}+anything\right]\cdot \mathcal{B}\left({P}_{c}^{+}\to pJ/\psi \right)\)</EquationSource> </InlineEquation> to be at the 10<sup><i>−</i>6</sup> level.</p>

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Search for a pentaquark state decaying into pJ/ψ in Υ(1, 2S) inclusive decays at Belle

  • X. Dong,
  • S. M. Zou,
  • H. Y. Zhang,
  • X. L. Wang,
  • I. Adachi,
  • J. K. Ahn,
  • H. Aihara,
  • S. Al Said,
  • D. M. Asner,
  • H. Atmacan,
  • R. Ayad,
  • S. Bahinipati,
  • Sw. Banerjee,
  • M. Bessner,
  • V. Bhardwaj,
  • D. Biswas,
  • D. Bodrov,
  • A. Bozek,
  • M. Bračko,
  • P. Branchini,
  • T. E. Browder,
  • A. Budano,
  • M. Campajola,
  • D. Červenkov,
  • M.-C. Chang,
  • P. Chang,
  • B. G. Cheon,
  • H. E. Cho,
  • K. Cho,
  • S.-K. Choi,
  • Y. Choi,
  • S. Choudhury,
  • S. Das,
  • G. De Nardo,
  • G. De Pietro,
  • R. Dhamija,
  • F. Di Capua,
  • J. Dingfelder,
  • Z. Doležal,
  • T. V. Dong,
  • P. Ecker,
  • D. Epifanov,
  • T. Ferber,
  • D. Ferlewicz,
  • B. G. Fulsom,
  • R. Garg,
  • V. Gaur,
  • A. Giri,
  • P. Goldenzweig,
  • E. Graziani,
  • T. Gu,
  • Y. Guan,
  • K. Gudkova,
  • C. Hadjivasiliou,
  • H. Hayashii,
  • S. Hazra,
  • M. T. Hedges,
  • W.-S. Hou,
  • C.-L. Hsu,
  • K. Inami,
  • N. Ipsita,
  • A. Ishikawa,
  • R. Itoh,
  • M. Iwasaki,
  • W. W. Jacobs,
  • S. Jia,
  • Y. Jin,
  • D. Kalita,
  • T. Kawasaki,
  • D. Y. Kim,
  • K.-H. Kim,
  • Y. J. Kim,
  • Y.-K. Kim,
  • K. Kinoshita,
  • P. Kodyš,
  • A. Korobov,
  • S. Korpar,
  • E. Kovalenko,
  • P. Križan,
  • P. Krokovny,
  • T. Kuhr,
  • R. Kumar,
  • T. Kumita,
  • A. Kuzmin,
  • Y.-J. Kwon,
  • Y.-T. Lai,
  • T. Lam,
  • J. S. Lange,
  • D. Levit,
  • L. K. Li,
  • Y. Li,
  • Y. B. Li,
  • L. Li Gioi,
  • J. Libby,
  • D. Liventsev,
  • Y. Ma,
  • M. Masuda,
  • T. Matsuda,
  • S. K. Maurya,
  • F. Meier,
  • M. Merola,
  • F. Metzner,
  • K. Miyabayashi,
  • R. Mussa,
  • I. Nakamura,
  • T. Nakano,
  • M. Nakao,
  • Z. Natkaniec,
  • A. Natochii,
  • L. Nayak,
  • M. Nayak,
  • S. Nishida,
  • S. Ogawa,
  • H. Ono,
  • G. Pakhlova,
  • S. Pardi,
  • H. Park,
  • J. Park,
  • S.-H. Park,
  • A. Passeri,
  • S. Patra,
  • S. Paul,
  • R. Pestotnik,
  • L. E. Piilonen,
  • T. Podobnik,
  • E. Prencipe,
  • M. T. Prim,
  • G. Russo,
  • S. Sandilya,
  • V. Savinov,
  • G. Schnell,
  • C. Schwanda,
  • Y. Seino,
  • K. Senyo,
  • M. E. Sevior,
  • W. Shan,
  • C. Sharma,
  • J.-G. Shiu,
  • J. B. Singh,
  • E. Solovieva,
  • M. Starič,
  • M. Takizawa,
  • K. Tanida,
  • F. Tenchini,
  • R. Tiwary,
  • M. Uchida,
  • Y. Unno,
  • S. Uno,
  • P. Urquijo,
  • Y. Usov,
  • A. Vinokurova,
  • S. Watanuki,
  • E. Won,
  • B. D. Yabsley,
  • W. Yan,
  • S. B. Yang,
  • J. Yelton,
  • J. H. Yin,
  • Y. Yook,
  • C. Z. Yuan,
  • L. Yuan,
  • Y. Yusa,
  • Z. P. Zhang,
  • V. Zhilich

摘要

Using the data samples of 102 million Υ(1S) and 158 million Υ(2S) events collected by the Belle detector, we search for a pentaquark state in the pJ/ψ final state from Υ(1, 2S) inclusive decays. Here, the charge-conjugate \(\overline{p }J/\psi \) is included. We observe clear pJ/ψ production in Υ(1, 2S) decays and measure the branching fractions to be \(\mathcal{B}[\Upsilon (1S)\to pJ/\psi +anything]=[8.1\pm 0.6(stat.)\pm 0.5(syst.)]\times {10}^{-5}\) and \(\mathcal{B}[\Upsilon (2S)\to pJ/\psi +anything]=[4.3\pm 0.5(stat.)\pm 0.4(syst.)]\times {10}^{-5}\) . We also measure the cross section of inclusive pJ/ψ production in e+e annihilation to be σ(e+epJ/ψ + anything) = [108 ± 11(stat.) ± 6(syst.)] fb at \(\sqrt{s}=10.52\) GeV using an 89.5 fb1 continuum data sample. There is no significant Pc(4312)+, Pc(4440)+ or Pc(4457)+ signal found in the pJ/ψ final states in Υ(1, 2S) inclusive decays. We determine the upper limits of \(\mathcal{B}\left[\Upsilon \left({1},{2}S\right)\to {P}_{c}^{+}+anything\right]\cdot \mathcal{B}\left({P}_{c}^{+}\to pJ/\psi \right)\) to be at the 106 level.