4.8 Article

Search for the Dark Photon and the Dark Higgs Boson at Belle

期刊

PHYSICAL REVIEW LETTERS
卷 114, 期 21, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.114.211801

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资金

  1. MEXT (Japan)
  2. JSPS (Japan)
  3. Nagoya's TLPRC (Japan)
  4. ARC (Australia)
  5. FWF (Austria)
  6. NSFC (China)
  7. MSMT (Czechia)
  8. CZF (Germany)
  9. DFG (Germany)
  10. VS (Germany)
  11. DST (India)
  12. INFN (Italy)
  13. MOE (Korea)
  14. MSIP (Korea)
  15. NRF (Korea)
  16. GSDC of KISTI (Korea)
  17. BK21Plus (Korea)
  18. MNiSW (Poland)
  19. NCN (Poland)
  20. MES (Russia)
  21. RFAAE (Russia)
  22. ARRS (Slovenia)
  23. IKERBASQUE (Spain)
  24. UPV/EHU (Spain)
  25. SNSF (Switzerland)
  26. NSC (Taiwan)
  27. MOE (Taiwan)
  28. U.S. DOE (USA)
  29. U.S. NSF (USA)

向作者/读者索取更多资源

The dark photon A' and the dark Higgs boson h' are hypothetical constituents featured in a number of recently proposed dark sector models. Assuming prompt decays of both dark particles, we search for their production in the so-called Higgstrahlung channel e(+)e(-) -> A'h', with h' -> A'A'. We investigate ten exclusive final states with A' -> e(+)e(-), mu(+)mu(-), or pi(+)pi(-) in the mass ranges 0.1 GeV/c(2) < m(A') < 3.5 GeV/c(2) and 0.2 GeV/c(2) < m(h') < 10.5 GeV/c(2). We also investigate three inclusive final states 2(e(+)e(-))X, 2(mu(+)mu(-))X, and (e(+)e(-))(mu(+)mu(-))X, where X denotes a dark photon candidate detected via missing mass, in the mass ranges 1.1 GeV/c(2) < m(A') < 3.5 GeV/c(2) and 2.2 GeV/c(2) < m(h') < 10.5 GeV/c(2). Using the entire 977 fb(-1) data set collected by Belle, we observe no significant signal. We obtain individual and combined 90% credibility level upper limits on the branching fraction times the Born cross section, B x sigma(Born), on the Born cross section sigma(Born), and on the dark photon coupling to the dark Higgs boson times the kinetic mixing between the standard model photon and the dark photon, alpha(D) x epsilon(2). These limits improve upon and cover wider mass ranges than previous experiments. The limits from the final states 3(pi(+)pi(-)) and 2(e(+)e(-))X are the first placed by any experiment. For alpha(D) equal to 1/137, m(h') < 8 GeV/c(2), and m(A') < 1 GeV/c(2), we exclude values of the mixing parameter epsilon above similar to 8 x 10(-4).

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