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Analysis of the nonleptonic charmonium modes Bs0→J/ψf2′(1525) and Bs0→J/ψK+K
In this work, we present an analysis of the nonleptonic charmonium modes Bs0→J/ψf2′(1525) and Bs0→J/ψK+K−. Within the framework of the factorization approach and using the perturbative QCD for the evaluation of the relevant form factors, we find a branching fraction for the two-body channel of BR(Bs...
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Published in: | Physical review. D 2017-02, Vol.95 (3), p.036013 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | In this work, we present an analysis of the nonleptonic charmonium modes Bs0→J/ψf2′(1525) and Bs0→J/ψK+K−. Within the framework of the factorization approach and using the perturbative QCD for the evaluation of the relevant form factors, we find a branching fraction for the two-body channel of BR(Bs0→J/ψf2′(1525))=(1.6−0.7+0.9)×10−4 which is in agreement with the experimental values reported by the LHCb and Belle Collaborations. The associated polarization fractions to this vector-tensor mode are also presented. On the other hand, nonresonant and resonant contributions to the three-body decay Bs0→J/ψK+K− are carefully investigated. The dominant contributions of the resonances ϕ(1020) and f2′(1525) are properly taken into account. A detailed analysis of the K+K− invariant mass distributions and Dalitz plot are also performed. The overall result BR(Bs0→J/ψK+K−)=(9.3−1.1+1.3)×10−4 is also in satisfactory agreement with the experimental information reported by LHCb and Belle. |
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ISSN: | 2470-0010 2470-0029 |
DOI: | 10.1103/PhysRevD.95.036013 |