Based on 4.481×108 ψ(3686) events collected with the BESIII detector at BEPCII, the branching fraction of the isospin violating decay ψ(3686)→ς¯0Λ+c.c. is measured to be (1.60±0.31±0.13±0.58)×10-6, where the first uncertainty is statistical, the second is systematic, and the third is the uncertainty arising from interference with the continuum. This result is significantly smaller than the measurement based on CLEO-c data sets. The decays χcJ→ΛΛ¯ are measured via ψ(3686)→γχcJ, and the branching fractions are determined to be B(χc0→ΛΛ¯)=(3.64±0.10±0.10±0.07)×10-4, B(χc1→ΛΛ¯)=(1.31±0.06±0.06±0.03)×10-4, B(χc2→ΛΛ¯)=(1.91±0.08±0.17±0.04)×10-4, where the third uncertainties are systematic due to the ψ(3686)→γχcJ branching fractions.

Measurements of the branching fractions of ψ(3686)→Σ¯0Λ+c.c. and χcJ(J=0,1,2)→ΛΛ¯

Garzia, I.;Scodeggio, M.;
2021

Abstract

Based on 4.481×108 ψ(3686) events collected with the BESIII detector at BEPCII, the branching fraction of the isospin violating decay ψ(3686)→ς¯0Λ+c.c. is measured to be (1.60±0.31±0.13±0.58)×10-6, where the first uncertainty is statistical, the second is systematic, and the third is the uncertainty arising from interference with the continuum. This result is significantly smaller than the measurement based on CLEO-c data sets. The decays χcJ→ΛΛ¯ are measured via ψ(3686)→γχcJ, and the branching fractions are determined to be B(χc0→ΛΛ¯)=(3.64±0.10±0.10±0.07)×10-4, B(χc1→ΛΛ¯)=(1.31±0.06±0.06±0.03)×10-4, B(χc2→ΛΛ¯)=(1.91±0.08±0.17±0.04)×10-4, where the third uncertainties are systematic due to the ψ(3686)→γχcJ branching fractions.
2021
Ablikim, M.; Achasov, M.  N.; Adlarson, P.; Ahmed, S.; Albrecht, M.; Aliberti, R.; Amoroso, A.; An, M.  R.; An, Q.; Bai, X.  H.; Bai, Y.; Bakina, O.; ...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11392/2506010
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