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Search for the dark photon in B 0 → A′A′, A′ → e + e , μ + μ , and π + π decays at Belle

  • The Belle Collaboration
  • Yonsei 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
  • Higher School of Economics
  • German Electron Synchrotron
  • Indian Institute of Technology Madras
  • University of Mississippi
  • University of Hawai'i at Mānoa
  • 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
  • University of Bonn
  • Fu Jen Catholic University
  • National Taiwan University
  • 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
  • Fudan University
  • RAS - Budker Institute of Nuclear Physics
  • Novosibirsk State University
  • University of Melbourne
  • Pacific Northwest National Laboratory

Research output: Contribution to journalArticlepeer-review

6 Scopus citations

Abstract

We present a search for the dark photon A′ in the B0 → A′A′ decays, where A′ subsequently decays to e+e, μ+μ, and π+π. The search is performed by analyzing 772 × 106BB¯ events collected by the Belle detector at the KEKB e+e energy-asymmetric collider at the ϒ(4S) resonance. No signal is found in the dark photon mass range 0.01 GeV/c2 ≤ mA′ ≤ 2.62 GeV/c2, and we set upper limits of the branching fraction of B0 → A′A′ at the 90% confidence level. The products of branching fractions, ℬ(B0→A′A′)×ℬ(A′→e+e−)2 and ℬ(B0→A′A′)×ℬ(A′→μ+μ−)2, have limits of the order of 10−8 depending on the A′ mass. Furthermore, considering A′ decay rate to each pair of charged particles, the upper limits of ℬ (B→ A′ A′) are of the order of 10−8–10−5. From the upper limits of ℬ (B→ A′ A′) , we obtain the Higgs portal coupling for each assumed dark photon and dark Higgs mass. The Higgs portal couplings are of the order of 10−2–10−1 at mh′≃mB0 ± 40 MeV/c2 and 10−1–1 at mh′≃mB0 ± 3 GeV/c2. [Figure not available: see fulltext.]

Original languageEnglish
Article number191
JournalJournal of High Energy Physics
Volume2021
Issue number4
DOIs
StatePublished - Apr 2021

Keywords

  • B physics
  • Beyond Standard Model
  • Rare decay
  • e+-e- Experiments

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