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The Bc -> BP,BV decays are studied with the QCD factorization approach (where P and V denote pseudoscalar and vector mesons, respectively). Considering the contributions of both current-current and penguin operators, the amplitudes of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Junfeng Sun , Yueling Yang , Wenjie Du , Huilan Ma

We study radiative decays of $\Upsilon$ to light quark jets in nonrelativistic QCD by taking both the color singlet and color octet $b\bar b$ operators into consideration. The cut for quark jet energy and cut for the angle between two quark…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ying-Jia Gao , Yu-Jie Zhang , Kuang-Ta Chao

Inspired by the recent LHCb measurements and forthcoming great potential on $B_{c}$ meson, we study the exclusive $B_{c}$ ${\to}$ $B_{q}P$, $B_{q}V$ decays with the perturbative QCD approach, where $q$ $=$ $u$, $d$, $s$; $P$ and $V$ denote…

High Energy Physics - Phenomenology · Physics 2015-06-22 Junfeng Sun , Yueling Yang , Qin Chang , Gongru Lu

Motivated by the experimental data, we study charmless $B_{u,d,s}\to VT$ ($V$ and $T$ denote light vector and tensor mesons respectively) decays in the perturbative QCD approach. The predictions of branching ratios, polarization fractions…

High Energy Physics - Phenomenology · Physics 2013-03-26 S. Freddy , C. S. Kim , R. H. Li , Z. T. Zou

Following the nonrelativistic QCD factorization scheme, by taking latest available measurement on $\chi_b(3P)$ into consideration, we present an updated study on the yield and polarization of $\Upsilon(1S,2S,3S)$ hadroproduction, and the…

High Energy Physics - Phenomenology · Physics 2015-10-20 Yu Feng , Bin Gong , Lu-Ping Wan , Jian-Xiong Wang

Theoretical predictions for inclusive semileptonic B decay rates are rewritten in terms of the Upsilon(1S) meson mass instead of the b quark mass, using a modified perturbation expansion. This method gives theoretically consistent and…

High Energy Physics - Phenomenology · Physics 2009-10-31 Andre H. Hoang , Zoltan Ligeti , Aneesh V. Manohar

In this paper we calculate the branching ratios (BRs) of the 32 charmless hadronic $B_c \to A P$ decays ($A=a_1(1260),b_1(1235),K_1(1270),K_1(1400), f_1(1285),f_1(1420),h_1(1170),h_1(1380)$) by employing the perturbative QCD(pQCD)…

High Energy Physics - Phenomenology · Physics 2010-04-22 Xin Liu , Zhen-Jun Xiao

In this paper, we calculate the decay rate and CP asymmetry of the $B_s \to \pi^+\pi^-$ decay in perturbative QCD approach with Sudakov resummation. Since none of the quarks in final states is the same as those of the initial $B_s$ meson,…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ying Li , Cai-Dian Lu , Zhen-Jun Xiao , Xian-Qiao Yu

Two-body charmless hadronic B decays involving a light tensor meson in the final states are studied in the perturbative QCD approach based on $k_T$ factorization. From our calculations, we find that the decay branching ratios for color…

High Energy Physics - Phenomenology · Physics 2013-05-30 Zhi-Tian Zou , Xin Yu , Cai-Dian Lu

In this talk I present the results of two calculations that make use of Non-Relativistic QCD and the newly developed Soft-Collinear Effective Theory. The first process considered is inclusive radiative $\Upsilon$ decay. The second process…

High Energy Physics - Phenomenology · Physics 2011-03-23 Sean Fleming

About 90% of Bs-bar Bs pairs produced at the Upsilon(5s) resonance are initially Bs*-bar Bs* pairs which decay radiatively to Bs-bar Bs. This implies that the Bs pair will then be in an eigenstate of charge conjugation (i.e. C=-1) and…

High Energy Physics - Phenomenology · Physics 2014-11-20 David Atwood , Amarjit Soni

We measure the ratio of branching fractions for the $\Upsilon (4S)$ decays to $B^+B^-$ and $B^0\bar{B}{}^0$ using $B^+ \rightarrow J/\psi(\ell\ell) K^+$ and $B^0 \rightarrow J/\psi(\ell\ell) K^0$ samples, where $J/\psi(\ell\ell)$ stands for…

High Energy Physics - Experiment · Physics 2023-02-28 Belle Collaboration , S. Choudhury , S. Sandilya , K. Trabelsi , A. Giri , I. Adachi , H. Aihara , D. M. Asner , H. Atmacan , T. Aushev , R. Ayad , V. Babu , S. Bahinipati , P. Behera , K. Belous , J. Bennett , M. Bessner , V. Bhardwaj , B. Bhuyan , T. Bilka , D. Bodrov , G. Bonvicini , J. Borah , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , D. Červenkov , M. -C. Chang , C. Chen , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , Y. Choi , D. Cinabro , S. Das , G. De Pietro , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , D. Epifanov , D. Ferlewicz , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , P. Goldenzweig , E. Graziani , T. Gu , K. Gudkova , C. Hadjivasiliou , T. Hara , K. Hayasaka , H. Hayashii , M. T. Hedges , D. Herrmann , W. -S. Hou , C. -L. Hsu , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , E. -J. Jang , Q. P. Ji , S. Jia , Y. Jin , K. K. Joo , K. H. Kang , T. Kawasaki , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , H. Kindo , K. Kinoshita , P. Kodyš , T. Konno , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , P. Krokovny , M. Kumar , R. Kumar , K. Kumara , Y. -J. Kwon , T. Lam , J. S. Lange , M. Laurenza , S. C. Lee , P. Lewis , J. Li , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , K. Lieret , D. Liventsev , T. Luo , M. Masuda , T. Matsuda , D. Matvienko , S. K. Maurya , F. Meier , M. Merola , F. Metzner , K. Miyabayashi , R. Mizuk , G. B. Mohanty , I. Nakamura , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , N. K. Nisar , S. Nishida , S. Ogawa , H. Ono , P. Oskin , P. Pakhlov , G. Pakhlova , S. Pardi , S. -H. Park , A. Passeri , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , S. Prell , E. Prencipe , M. T. Prim , N. Rout , G. Russo , Y. Sakai , A. Sangal , L. Santelj , V. Savinov , J. Schueler , C. Schwanda , A. J. Schwartz , Y. Seino , K. Senyo , M. E. Sevior , M. Shapkin , C. Sharma , C. P. Shen , J. -G. Shiu , J. B. Singh , A. Sokolov , E. Solovieva , M. Starič , Z. S. Stottler , J. F. Strube , M. Sumihama , T. Sumiyoshi , M. Takizawa , K. Tanida , F. Tenchini , M. Uchida , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Ushiroda , Y. Usov , R. van Tonder , G. Varner , K. E. Varvell , A. Vinokurova , A. Vossen , E. Waheed , E. Wang , M. -Z. Wang , X. L. Wang , M. Watanabe , S. Watanuki , E. Won , X. Xu , B. D. Yabsley , S. B. Yang , J. Yelton , J. H. Yin , C. Z. Yuan , Y. Yusa , Y. Zhai , Z. P. Zhang , V. Zhilich , V. Zhukova

We study two-body hadronic $B_s\to PT$ decays, with $P (T)$ being a light pseudoscalar (tensor) meson, in the perturbative QCD approach. The CP-averaged branching ratios and the direct CP asymmetries of the $\Delta S=0$ modes are predicted,…

High Energy Physics - Phenomenology · Physics 2014-03-25 Qin Qin , Zhi-Tian Zou , Xin Yu , Hsiang-nan Li , Cai-Dian Lü

The nonleptonic two body $B_{u,d,s,c}$ decays involving a light tensor meson in final states are studied in the perturbative QCD approach based on $k_T$ factorization. The decay modes with a tensor meson emitted, are prohibited in naive…

High Energy Physics - Phenomenology · Physics 2014-01-08 Zhi-Tian Zou , Cai-Dian Lu

The recent measurements by CLEO Collaboration for the inclusive J/Psi and Psi(2S) production in Upsilon(1S) decay and our previous calculation are analyzed. The J/Psi momentum spectrum and the production ratio of Psi(2S) versus J/Psi favour…

High Energy Physics - Phenomenology · Physics 2011-03-23 Wei Han , Shi-Yuan Li

In this work, we explore the $P$-wave resonance contributions to the three-body charmonium decays of $B_c\to \Psi (V\to) P_1P_2$ using the perturbative QCD formalism at leading order, where $\Psi$ denotes a $S$-wave charmonium state, such…

High Energy Physics - Phenomenology · Physics 2026-05-11 Jia-Ying Wang , Jing Jiang , Yu-Jie Liu , Da-Cheng Yan , Zhou Rui , Zhen-Jun Xiao , Ya Li

We study the $B(B_{s})\rightarrow D_{(s)}(\bar{D}_{(s)})\,T$ and $D_{(s)}^{\ast}(\bar{D}_{(s)}^{*})\,T$ decays in perturbative QCD approach, where T denotes a light tensor meson. In addition to the branching ratios, we also give predictions…

High Energy Physics - Phenomenology · Physics 2012-09-18 Zhi-Tian Zou , Xin Yu , Cai-Dian Lu

We study two-body weak hadronic decays of \psi and Upsilon employing the factorization scheme. Branching ratios for \psi -> PP/PV and \Upsilon -> PP/PV decays in the Cabibbo-angle-enhanced and Cabibbo-angle-suppressed modes are predicted.

High Energy Physics - Phenomenology · Physics 2009-10-31 K. K. Sharma , R. C. Verma

The potential of a Super Flavor Factory (SFF) for searches of New Physics is reviewed. While very high luminosity B physics is assumed to be at the core of the program, its scope for extensive charm and tau studies are also emphasized. The…

High Energy Physics - Phenomenology · Physics 2014-11-18 Thomas E. Browder , Tim Gershon , Dan Pirjol , Amarjit Soni , Jure Zupan

In this paper, we will make systematic calculations for the branching ratios and the CP-violating asymmetries of the twenty one $\bar{B}^0_s \to PV $ decays by employing the perturbative QCD (PQCD) factorization approach. Besides the full…

High Energy Physics - Phenomenology · Physics 2018-05-09 Da-Cheng Yan , Ping Yang , Xin Liu , Zhen-Jun Xiao