TY - JOUR
T1 - Observation and branching fraction measurement of the decay Ξ−b→Λ0bπ−
AU - LHCb Collaboration
AU - Bifani, Simone
AU - Calladine, Ryan
AU - Cooke, Naomi
AU - Lazzeroni, Cristina
AU - Plews, Jonathan
AU - Sahoo, Niladribihari
AU - Slater, Mark
AU - Swallow, Paul
AU - Thompson, D. J. D.
AU - Watson, Nigel
PY - 2023/10/6
Y1 - 2023/10/6
N2 - The decay Ξ−b→Λ0bπ− is observed using a proton-proton collision data sample collected at center-of-mass energy s√=13 TeV with the LHCb detector, corresponding to an integrated luminosity of 5.5 fb−1. This process is mediated by the s→uu¯d quark-level transition, where the b quark in the Ξ−b baryon is a spectator in the decay. Averaging the results obtained using the two Λ0b decay modes, Λ0b→Λ+cπ− and Λ0b→Λ+cπ−π+π−, the relative production ratio is measured to be (fΞ−b/fΛ0b)B(Ξ−b→Λ0bπ−)=(7.3±0.8±0.6)×10−4. Here the uncertainties are statistical and systematic, respectively, and fΞ−b(fΛ0b) is the fragmentation fraction for a b quark into a Ξ−b (Λ0b) baryon. Using an independent measurement of fΞ−b/fΛ0b, the branching fraction B(Ξ−b→Λ0bπ−)=(0.89±0.10±0.07±0.29)% is obtained, where the last uncertainty is due to the assumed SU(3) flavor symmetry in the determination of fΞ−b/fΛ0b.
AB - The decay Ξ−b→Λ0bπ− is observed using a proton-proton collision data sample collected at center-of-mass energy s√=13 TeV with the LHCb detector, corresponding to an integrated luminosity of 5.5 fb−1. This process is mediated by the s→uu¯d quark-level transition, where the b quark in the Ξ−b baryon is a spectator in the decay. Averaging the results obtained using the two Λ0b decay modes, Λ0b→Λ+cπ− and Λ0b→Λ+cπ−π+π−, the relative production ratio is measured to be (fΞ−b/fΛ0b)B(Ξ−b→Λ0bπ−)=(7.3±0.8±0.6)×10−4. Here the uncertainties are statistical and systematic, respectively, and fΞ−b(fΛ0b) is the fragmentation fraction for a b quark into a Ξ−b (Λ0b) baryon. Using an independent measurement of fΞ−b/fΛ0b, the branching fraction B(Ξ−b→Λ0bπ−)=(0.89±0.10±0.07±0.29)% is obtained, where the last uncertainty is due to the assumed SU(3) flavor symmetry in the determination of fΞ−b/fΛ0b.
U2 - 10.1103/PhysRevD.108.072002
DO - 10.1103/PhysRevD.108.072002
M3 - Article
SN - 1550-7998
VL - 108
JO - Physical Review D - Particles, Fields, Gravitation and Cosmology
JF - Physical Review D - Particles, Fields, Gravitation and Cosmology
M1 - 072002
ER -