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Quasi-two-body decays B→Kρ→Kππ in perturbative QCD approach
We analyze the quasi-two-body decays B→Kρ→Kππ in the perturbative QCD (PQCD) approach, in which final-state interactions between the pions in the resonant regions associated with the P-wave states ρ(770) and ρ′(1450) are factorized into two-pion distribution amplitudes. Adopting experimental inputs...
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Published in: | Physics letters. B 2016-12, Vol.763, p.29-39 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We analyze the quasi-two-body decays B→Kρ→Kππ in the perturbative QCD (PQCD) approach, in which final-state interactions between the pions in the resonant regions associated with the P-wave states ρ(770) and ρ′(1450) are factorized into two-pion distribution amplitudes. Adopting experimental inputs for the time-like pion form factors involved in two-pion distribution amplitudes, we calculate branching ratios and direct CP asymmetries of the B→Kρ(770),Kρ′(1450)→Kππ modes. It is shown that agreement of theoretical results with data can be achieved, through which Gegenbauer moments of the P-wave two-pion distribution amplitudes are determined. The consistency between the three-body and two-body analyses of the B→Kρ(770)→Kππ decays supports the PQCD factorization framework for exclusive hadronic B meson decays. |
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ISSN: | 0370-2693 1873-2445 |
DOI: | 10.1016/j.physletb.2016.10.026 |