The nonleptonic two body B decays involving a light tensor meson in final states  

作　　者：Zhi-Tian Zou Cai-Dian L 

机构地区：[1]Department of Physics,Yantai University [2]Institute of High Energy Physics and Theoretical Physics Center for Science Facilities,Chinese Academy of Sciences

出　　处：《Chinese Science Bulletin》2014年第29期3738-3747,共10页

基　　金：supported in part by the Foundation of Yantai University (WL07052);the National Natural Science Foundation of China (11375208,11228512,11235005 and 11175151)

摘　　要：The nonleptonic two body Bu;d;s;c decays involving a light tensor meson in final states are studied in the perturbative QCD approach based on kTfactorization.The decay modes with a tensor meson emitted,are prohibited in naive factorization,since the emission diagram with a tensor meson produced from vacuum is vanished.While contributions from the so-called hard scattering emission diagrams and annihilation type diagrams are important and calculable in the perturbative QCD approach.The branching ratios of most decays are in the range of 10 4–10 8,which are bigger by 1 or 2 orders of magnitude than the predictions given by the naive factorization,but consistent with the predictions from the QCD factorization and the recent experimental measurements.We also give the predictions for the direct CP asymmetries,some of which are large enough for the future experiments to measure.We also find that,even with a small mixing angle,the mixing between f2and f02can bring remarkable changes to both branching ratios and the direct CP asymmetries for some decays involving fe0T2mesons.For decays with a vector meson and a tensor meson in final states,we predict a large percentage of transverse polarization contributions due to the contributions of the orbital angular momentum of the tensor mesons.The nonleptonic two body Bu,d,s,c decays involving a light tensor meson in final states are studied in the perturbative QCD approach based on kT factorization. The decay modes with a tensor meson emitted, are prohibited in naive factorization, since the emission diagram with a tensor meson produced from vacuum is vanished. While contributions from the so-called hard scattering emission diagrams and annihilation type diagrams are important and calculable in the perturbative QCD approach. The branching ratios of most decays are in the range of 10-4-10-8, which are bigger by 1 or 2 orders of magnitude than the predictions given by the naive factor- ization, but consistent with the predictions from the QCD factorization and the recent experimental measurements. We also give the predictions for the direct CP asymmetries, some of which are large enough for the future experiments to measure. We also find that, even with a small mixing angle, the mixing between f2 and f′2 can bring remarkable changes to both branching ratios and the direct CP asymmetries for some decays involving f2（′） mesons. For decays with a vector meson and a tensor meson in final states, we predict a large percentage of transverse polarization contributions due to the contributions of the orbital angular momentum of the tensor mesons.

关 键 词：矢量介子 B衰变 张量 终态 车身 微扰QCD 实验测量 衰减模式 

分 类 号：O572.33[理学—粒子物理与原子核物理]