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Study of γγ →γψ (2S) at Belle

  • (Belle Collaboration)
  • University of the Basque Country
  • Fudan University
  • The Graduate University for Advanced Studies
  • High Energy Accelerator Research Organization, Tsukuba
  • The University of Tokyo
  • King Abdulaziz University
  • University of Tabuk
  • Brookhaven National Laboratory
  • University of Cincinnati
  • RAS - Budker Institute of Nuclear Physics
  • Novosibirsk State University
  • Higher School of Economics
  • German Electron Synchrotron
  • Indian Institute of Technology Bhubaneswar
  • Indian Institute of Technology Madras
  • Indian Institute of Science Education and Research Mohali
  • Indian Institute of Technology Guwahati
  • Charles University
  • Jožef Stefan Institute
  • Wayne State University
  • H. Niewodniczanski Institute of Nuclear Physics
  • University of Maribor
  • National Institute for Nuclear Physics
  • University of Naples Federico II
  • Fu Jen Catholic University
  • Max Planck Institute for Physics (Werner Heisenberg Institute)
  • National Central University
  • Hanyang University
  • RAS - P.N. Lebedev Physics Institute
  • Korea Institute of Science and Technology Information
  • Gyeongsang National University
  • Sungkyunkwan University
  • Indian Institute of Technology Hyderabad
  • Malaviya National Institute of Technology
  • University of Melbourne
  • University of Göttingen
  • Pacific Northwest National Laboratory
  • Panjab University

Research output: Contribution to journalArticlepeer-review

32 Scopus citations

Abstract

Using 980 fb-1 of data at and around the I (nS) (n=1, 2, 3, 4, 5) resonances collected with the Belle detector at the KEKB asymmetric-energy e+e-collider, the two-photon process γγ→γψ(2S) is studied from the threshold to 4.2 GeV for the first time. Two structures are seen in the invariant mass distribution of γψ(2S): one at MR1=3922.4±6.5±2.0 MeV/c2 with a width of ΓR1=22±17±4 MeV, and another at MR2=4014.3±4.0±1.5 MeV/c2 with a width of ΓR2=4±11±6 MeV; the signals are parametrized with the incoherent sum of two Breit-Wigner functions. The first structure is consistent with the X(3915) or the χc2(3930), and the local statistical significance is determined to be 3.1σ with the systematic uncertainties included. The second matches none of the known charmonium or charmoniumlike states, and its global significance is determined to be 2.8σ including the look-elsewhere effect. The production rates are ΓγγB(R1→γψ(2S))=9.8±3.6±1.3 eV assuming (JPC,|λ|)=(0++,0) or 2.0±0.7±0.2 eV with (2++,2) for the first structure and ΓγγB(R2→γψ(2S))=6.2±2.2±0.8 eV with (0++,0) or 1.2±0.4±0.2 eV with (2++,2) for the second. Here, the first errors are statistical and the second systematic, and λ is the helicity.

Original languageEnglish
Article number112011
JournalPhysical Review D
Volume105
Issue number11
DOIs
StatePublished - 1 Jun 2022

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