B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) Decays in QCD Factorization Approach

The hadronic B → J / ψ K ( 1270 ) and B →...

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Main Authors: Mahboobeh Sayahi, Hossein Mehraban
Format: Article
Language:English
Published: Wiley 2012-01-01
Series:Advances in High Energy Physics
Online Access:http://dx.doi.org/10.1155/2012/494031
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author Mahboobeh Sayahi
Hossein Mehraban
author_facet Mahboobeh Sayahi
Hossein Mehraban
author_sort Mahboobeh Sayahi
collection DOAJ
description The hadronic B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) has been analyzed in “QCD factorization” approach and generalized factorization. The effective coefficients a i h have been calculated for three helicity states h = 0 , + , − which give three different contribution of amplitudes. We consider that J/ψ behaves as a light meson in compared to B meson. For B + → J / ψ K + ( 1270 ) and B + → J / ψ K + ( 1400 ) , experimental data of branching ratios are (1.8 ± 0.5) × 10−3 and <5 × 10−4, respectively. Our best obtained results are (1.79 ± 0.01) × 10−3 at θ = 58° and (1.42 ± 0.01) × 10−3 at θ = 32° for B + → J / ψ K + ( 1270 ) decay. And we have 4.27 × 10−4 at θ = 58° and 3.45 × 10−4 at θ = 32° for B + → J / ψ K + ( 1400 ) , which are in agreement with experiment.
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spelling doaj-art-ddd98b575fcf4b2e9f286416049796f82025-02-03T05:44:54ZengWileyAdvances in High Energy Physics1687-73571687-73652012-01-01201210.1155/2012/494031494031B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) Decays in QCD Factorization ApproachMahboobeh Sayahi0Hossein Mehraban1Physics Department, Semnan University, P.O. Box 35195-363, Semnan 35351, IranPhysics Department, Semnan University, P.O. Box 35195-363, Semnan 35351, IranThe hadronic B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) has been analyzed in “QCD factorization” approach and generalized factorization. The effective coefficients a i h have been calculated for three helicity states h = 0 , + , − which give three different contribution of amplitudes. We consider that J/ψ behaves as a light meson in compared to B meson. For B + → J / ψ K + ( 1270 ) and B + → J / ψ K + ( 1400 ) , experimental data of branching ratios are (1.8 ± 0.5) × 10−3 and <5 × 10−4, respectively. Our best obtained results are (1.79 ± 0.01) × 10−3 at θ = 58° and (1.42 ± 0.01) × 10−3 at θ = 32° for B + → J / ψ K + ( 1270 ) decay. And we have 4.27 × 10−4 at θ = 58° and 3.45 × 10−4 at θ = 32° for B + → J / ψ K + ( 1400 ) , which are in agreement with experiment.http://dx.doi.org/10.1155/2012/494031
spellingShingle Mahboobeh Sayahi
Hossein Mehraban
B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) Decays in QCD Factorization Approach
Advances in High Energy Physics
title B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) Decays in QCD Factorization Approach
title_full B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) Decays in QCD Factorization Approach
title_fullStr B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) Decays in QCD Factorization Approach
title_full_unstemmed B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) Decays in QCD Factorization Approach
title_short B → J / ψ K ( 1270 ) and B → J / ψ K ( 1400 ) Decays in QCD Factorization Approach
title_sort b j ψ k 1270 and b j ψ k 1400 decays in qcd factorization approach
url http://dx.doi.org/10.1155/2012/494031
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