Non-leptonic two-body decays of Λb0 in light-front quark model
We study the non-leptonic two-body weak decays of Λb0→pM with M=(π−,K−) and (ρ−,K⁎−) in the light-front quark model under the generalized factorization ansatz. By considering the Fermi statistic between quarks and determining spin-flavor structures in baryons, we calculate the branching ratios (Bs)...
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2021-04-01
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doaj-afdd31008bce4c3d8078d7f6850cbd0d2021-03-22T12:35:17ZengElsevierPhysics Letters B0370-26932021-04-01815136125Non-leptonic two-body decays of Λb0 in light-front quark modelC.Q. Geng0Chia-Wei Liu1Tien-Hsueh Tsai2School of Fundamental Physics and Mathematical Sciences, Hangzhou Institute for Advanced Study, UCAS, Hangzhou 310024, China; International Centre for Theoretical Physics Asia-Pacific, Beijing/Hangzhou, China; Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan; Physics Division, National Center for Theoretical Sciences, Hsinchu 300, Taiwan; Corresponding author.Department of Physics, National Tsing Hua University, Hsinchu 300, TaiwanDepartment of Physics, National Tsing Hua University, Hsinchu 300, TaiwanWe study the non-leptonic two-body weak decays of Λb0→pM with M=(π−,K−) and (ρ−,K⁎−) in the light-front quark model under the generalized factorization ansatz. By considering the Fermi statistic between quarks and determining spin-flavor structures in baryons, we calculate the branching ratios (Bs) and CP-violating rate asymmetries (ACPs) in the decays. Explicitly, we find that B(Λb0→pπ−,pK−)=(4.18±0.15±0.30,5.76±0.88±0.23)×10−6 and ACP(Λb0→pπ−,pK−)=(−3.60±0.14±0.14,6.36±0.21±0.18)% in comparison with the data of B(Λb0→pπ−,pK−)=(4.5±0.8,5.4±1.0)×10−6 and ACP(Λb0→pπ−,pK−)=(−2.5±2.9,−2.5±2.2)% given by the Particle Data Group, respectively. We also predict that B(Λb0→pρ−,pK⁎−)=(12.13±3.27±0.91,2.58±0.87±0.13)×10−6 and ACP(Λb0→pρ−,pK⁎−)=(−3.32±0.00±0.14,19.25±0.00±0.80)%, which could be observed by the experiments at LHCb.http://www.sciencedirect.com/science/article/pii/S0370269321000654 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
C.Q. Geng Chia-Wei Liu Tien-Hsueh Tsai |
spellingShingle |
C.Q. Geng Chia-Wei Liu Tien-Hsueh Tsai Non-leptonic two-body decays of Λb0 in light-front quark model Physics Letters B |
author_facet |
C.Q. Geng Chia-Wei Liu Tien-Hsueh Tsai |
author_sort |
C.Q. Geng |
title |
Non-leptonic two-body decays of Λb0 in light-front quark model |
title_short |
Non-leptonic two-body decays of Λb0 in light-front quark model |
title_full |
Non-leptonic two-body decays of Λb0 in light-front quark model |
title_fullStr |
Non-leptonic two-body decays of Λb0 in light-front quark model |
title_full_unstemmed |
Non-leptonic two-body decays of Λb0 in light-front quark model |
title_sort |
non-leptonic two-body decays of λb0 in light-front quark model |
publisher |
Elsevier |
series |
Physics Letters B |
issn |
0370-2693 |
publishDate |
2021-04-01 |
description |
We study the non-leptonic two-body weak decays of Λb0→pM with M=(π−,K−) and (ρ−,K⁎−) in the light-front quark model under the generalized factorization ansatz. By considering the Fermi statistic between quarks and determining spin-flavor structures in baryons, we calculate the branching ratios (Bs) and CP-violating rate asymmetries (ACPs) in the decays. Explicitly, we find that B(Λb0→pπ−,pK−)=(4.18±0.15±0.30,5.76±0.88±0.23)×10−6 and ACP(Λb0→pπ−,pK−)=(−3.60±0.14±0.14,6.36±0.21±0.18)% in comparison with the data of B(Λb0→pπ−,pK−)=(4.5±0.8,5.4±1.0)×10−6 and ACP(Λb0→pπ−,pK−)=(−2.5±2.9,−2.5±2.2)% given by the Particle Data Group, respectively. We also predict that B(Λb0→pρ−,pK⁎−)=(12.13±3.27±0.91,2.58±0.87±0.13)×10−6 and ACP(Λb0→pρ−,pK⁎−)=(−3.32±0.00±0.14,19.25±0.00±0.80)%, which could be observed by the experiments at LHCb. |
url |
http://www.sciencedirect.com/science/article/pii/S0370269321000654 |
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