4.7 Article

Measurements of B((B)over-bar0 → Λc+(p)over-bar and B(B- → Λc+(p)over-barπ-) and studies of Λc+π- resonances

期刊

PHYSICAL REVIEW D
卷 78, 期 11, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.78.112003

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资金

  1. U. S. Department of Energy and National Science Foundation
  2. Natural Sciences and Engineering Research Council (Canada)
  3. Commissariat a l'Energie Atomique and Institut National de Physique Nucleaire et de Physique des Particules (France)
  4. Bundesministerium fur Bildung und Forschung and Deutsche Forschungsgemeinschaft (Germany)
  5. Istituto Nazionale di Fisica Nucleare (Italy)
  6. Foundation for Fundamental Research on Matter (The Netherlands)
  7. Research Council of Norway
  8. Ministry of Education and Science of the Russian Federation
  9. Ministerio de Educacion y Ciencia (Spain)
  10. Science and Technology Facilities Council (United Kingdom)
  11. Marie-Curie IEF program (European Union)
  12. A. P. Sloan Foundation
  13. STFC [ST/F008015/1] Funding Source: UKRI
  14. Science and Technology Facilities Council [ST/F008015/1, PP/E000444/1] Funding Source: researchfish

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We present an investigation of the decays B-0 -> Lambda(+)(c)(p) over bar and B- -> Lambda(+)(c)(p) over bar pi(-) based on 383 X 10(6)Y(4S) -> B (B) over bar decays recorded with the BABAR detector. We measure the branching fractions of these decays; their ratio is B(B- -> Lambda(+)(c)(p) over bar pi(-))/B((B) over bar (0) -> Lambda(+)(c)(p) over bar) = 15.4 +/- 1.8 +/- 0.3. The B- -> Lambda(+)(c)(p) over bar pi(-) process exhibits an enhancement at the Lambda(+)(c)(p) over bar threshold and is a laboratory for searches for excited charm baryon states. We observe the resonant decays B- -> Sigma(c)(2455)(0)(p) over bar and B- -> Sigma(c)(2800)(0)(p) over bar but see no evidence for B- -> Sigma(c)(2520)(0)(p) over bar. This is the first observation of the decay B- -> Sigma(c)(2800)(0)(p) over bar; however, the mass of the observed excited Sigma(0)(c) state is (2846 +/- 8 +/- 10) MeV/c(2), which is somewhat inconsistent with previous measurements. Finally, we examine the angular distribution of the B- -> Sigma(c)(2455)(0)(p) over bar decays and measure the spin of the Sigma(c)(2455)(0) baryon to be 1/2, as predicted by the quark model.

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