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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Main Authors: C.Q. Geng, Chia-Wei Liu, Tien-Hsueh Tsai
Format: Article
Language:English
Published: Elsevier 2021-04-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269321000654
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spelling 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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