4.7 Article

First branching fraction measurement of the suppressed decay Ξc0 → π- Λc+

期刊

PHYSICAL REVIEW D
卷 102, 期 7, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.102.071101

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资金

  1. CERN
  2. CAPES (Brazil)
  3. CNPq (Brazil)
  4. FAPERJ (Brazil)
  5. FINEP (Brazil)
  6. MOST (China)
  7. NSFC (China)
  8. CNRS/IN2P3 (France)
  9. BMBF (Germany)
  10. DFG (Germany)
  11. MPG (Germany)
  12. INFN (Italy)
  13. NWO (Netherlands)
  14. MNiSW (Poland)
  15. NCN (Poland)
  16. MEN/IFA (Romania)
  17. MSHE (Russia)
  18. MinECo (Spain)
  19. SNSF (Switzerland)
  20. SER (Switzerland)
  21. NASU (Ukraine)
  22. STFC (United Kingdom)
  23. DOE NP (USA)
  24. NSF (USA)
  25. AvH Foundation (Germany)
  26. EPLANET (European Union)
  27. Marie Sklodowska-Curie Actions (European Union)
  28. ERC (European Union)
  29. A*MIDEX (France)
  30. ANR (France)
  31. Labex P2IO (France)
  32. Labex OCEVU (France)
  33. Region Auvergne-Rhone-Alpes (France)
  34. Key Research Program of Frontier Sciences of CAS (China)
  35. CAS PIFI (China)
  36. Thousand Talents Program (China)
  37. RFBR (Russia)
  38. RSF (Russia)
  39. Yandex LLC (Russia)
  40. GVA (Spain)
  41. XuntaGal (Spain)
  42. GENCAT (Spain)
  43. Royal Society (United Kingdom)
  44. Leverhulme Trust (United Kingdom)
  45. STFC [ST/S000879/1, ST/S000739/1, ST/S000909/1, LHCb, ST/S000801/1] Funding Source: UKRI

向作者/读者索取更多资源

The Xi(0)(c) baryon is unstable and usually decays into charmless final states by the c -> sud transition. It can, however, also disintegrate into a pi(-) meson and a Lambda(+)(c) baryon via s quark decay or via cs -> dc weak scattering. The interplay between the latter two processes governs the size of the branching fraction B(Xi(0)(c) -> pi(-) Lambda(+)(c)), first measured here to be (0.55 +/- 0.02 +/- 0.18)%, where the first uncertainty is statistical and second systematic. This result is compatible with the larger of the theoretical predictions that connect models of hyperon decays using partially conserved axial currents and SU(3) symmetry with those involving the heavy-quark expansion and heavy-quark symmetry. In addition, the branching fraction of the normalization channel, B(Xi(+)(c) -> pK(-) pi(+)) = (1.135 +/- 0.002 +/- 0.387)% is measured.

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