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We will present a review of the most interesting results on rare B decays from the B Factories, based on the data collected by the BaBar and Belle detectors at asymmetric $e^+ e^-$ colliders at the center of mass energy of the…

High Energy Physics - Experiment · Physics 2009-05-18 Elisabetta Baracchini

This article is devoted to systematic analysis of double charmonium production in exclusive $Z$ boson decays in the framework of Nonrelativistic Quantum Chromodynamic (NRQCD) and leading twist light-cone (LC) models. Theoretical predictions…

High Energy Physics - Phenomenology · Physics 2018-05-23 A. K. Likhoded , A. V. Luchinsky

My report consists of two parts: (1). Using samples of 102 million $\Upsilon(1S)$ and 158 million $\Upsilon(2S)$ events at Belle, we study 17 exclusive hadronic decays of these two bottomonium resonances to some Vector-Pseudoscalar (VP),…

High Energy Physics - Experiment · Physics 2019-08-21 Chengping Shen

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

Motivated by very recent measurement of the radiative decays of $\Upsilon(1S)$ to $\chi_{c1}$ at Belle, we use the nonrelativistic QCD factorization theory and calculate the branching fractions of the radiative decays of bottomonium into…

High Energy Physics - Phenomenology · Physics 2020-11-10 Dan-Dan Shen , Chong-Yang Lu , Peng Sun , Ruilin Zhu

Using data collected by the CLEO III detector at CESR, we started a series of investigations on the Upsilon(5S) resonance decay properties. The data sample used for this analysis consists of 0.42 fb-1 of data taken on the Upsilon(5S)…

High Energy Physics - Experiment · Physics 2015-06-25 D. M. Asner , CLEO Collaboration

We observe the process $\Upsilon(2S)\to D_s^{(*)+} D_{sJ}^{-}$ and continuum production $e^+e^- \to D_s^{(*)+} D_{sJ}^- $ at $\sqrt{s} = 10.52$ GeV (and their charge conjugates) using the data samples collected by the Belle detector at…

High Energy Physics - Experiment · Physics 2023-08-23 Belle Collaboration , B. S. Gao , W. J. Zhu , X. L. Wang , I. Adachi , H. Aihara , D. M. Asner , V. Aulchenko , T. Aushev , R. Ayad , V. Babu , Sw. Banerjee , M. Bauer , P. Behera , K. Belous , J. Bennett , M. Bessner , V. Bhardwaj , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , A. Bondar , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , D. Červenkov , M. -C. Chang , P. Chang , V. Chekelian , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , G. De Nardo , G. De Pietro , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , P. Ecker , T. Ferber , D. Ferlewicz , B. G. Fulsom , V. Gaur , A. Giri , E. Graziani , T. Gu , K. Gudkova , C. Hadjivasiliou , K. Hayasaka , H. Hayashii , S. Hazra , M. T. Hedges , D. Herrmann , W. -S. Hou , C. -L. Hsu , T. Iijima , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , E. -J. Jang , S. Jia , Y. Jin , K. K. Joo , T. Kawasaki , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , T. Konno , A. Korobov , S. Korpar , P. Križan , M. Kumar , R. Kumar , K. Kumara , A. Kuzmin , Y. -J. Kwon , Y. -T. Lai , S. C. Lee , D. Levit , P. Lewis , L. K. Li , L. Li Gioi , J. Libby , K. Lieret , D. Liventsev , Y. Ma , M. Masuda , T. Matsuda , S. K. Maurya , F. Meier , M. Merola , R. Mizuk , I. Nakamura , M. Nakao , D. Narwal , A. Natochii , L. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , S. Ogawa , P. Pakhlov , G. Pakhlova , S. Pardi , J. Park , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , E. Prencipe , M. T. Prim , G. Russo , S. Sandilya , V. Savinov , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , W. Shan , C. Sharma , J. -G. Shiu , B. Shwartz , E. Solovieva , M. Starič , Z. S. Stottler , M. Sumihama , K. Tanida , F. Tenchini , M. Uchida , T. Uglov , Y. Unno , S. Uno , S. E. Vahsen , K. E. Varvell , D. Wang , E. Wang , M. -Z. Wang , S. Watanuki , E. Won , X. Xu , B. D. Yabsley , W. Yan , S. B. Yang , J. H. Yin , Y. Yook , C. Z. Yuan , L. Yuan , V. Zhilich , V. Zhukova

A sample of 3.79 million psi(2S) decays observed in the BES detector is used to study the decays of charmonium to axialvector plus pseudoscalar mesons. The branching fraction for psi(2S) to b1pi agrees with expectations. A contrasting…

High Energy Physics - Experiment · Physics 2008-11-26 BES Collaboration , J. Z. Bai

The strong, electromagnetic and mixed strong-electromagnetic amplitudes of the $\psi(2S)$ decays into baryon-anti-baryon pairs have been obtained by exploiting all available data sets in the framework of an effective Lagrangian model. We…

High Energy Physics - Phenomenology · Physics 2021-01-13 Rinaldo Baldini Ferroli , Alessio Mangoni , Simone Pacetti , Kai Zhu

We report the first observation of e+e- -> Upsilon(1S)pi+pi-, Upsilon(2S)pi+pi-, and first evidence for e+e- -> Upsilon(3S)pi+pi-, Upsilon(1S)K+K-, near the peak of the Upsilon(5S) resonance at sqrt{s}~10.87 GeV. The results are based on a…

High Energy Physics - Experiment · Physics 2009-10-26 The Belle Collaboration , K. -F. Chen , W. -S. Hou , M. Shapkin , A. Sokolov et al

We address Standard Model predictions for flavor-changing radiative transitions of the pseudoscalar charm mesons. Short-distance contributions in $D$ radiative transitions are contrasted with those in B decays. A full analysis is presented…

High Energy Physics - Phenomenology · Physics 2010-04-06 Gustavo Burdman , Eugene Golowich , JoAnne L. Hewett , Sandip Pakvasa

By analyzing existing data on pseudoscalar charmonium decays, we obtain the ratio of the branching fractions of $\eta_c(2S)$ and $\eta_c$ decays into ten different final states with light hadrons. For the first time, we test the two…

High Energy Physics - Phenomenology · Physics 2022-05-17 Hongpeng Wang , Chang-Zheng Yuan

Using data collected using the CLEO III detector, we present recent results on decays of the $\Upsilon(1S)-\Upsilon(3S)$ resonances. We report on three analyses. They are: (1) improved measurements of the muonic branching fraction of the…

High Energy Physics - Experiment · Physics 2019-08-14 Steven R. Blusk

Motivated by the prospects of the potential ${\Upsilon}(1S)$ particle at high-luminosity heavy-flavor experiments, we studied the ${\Upsilon}(1S)$ ${\to}$ $B_{c}M$ weak decays, where $M$ $=$ ${\pi}$, ${\rho}$, $K^{(\ast)}$. The…

High Energy Physics - Phenomenology · Physics 2016-10-24 Junfeng Sun , Lili Chen , Na Wang , Qin Chang , Jinshu Huang , Yueling Yang

We present a measurement of the branching fraction of invisible Upsilon(1S) decays, using 1.2 fb^{-1} of data collected at the Upsilon(2S) resonance with the CLEO III detector at CESR. After subtracting expected backgrounds from events that…

High Energy Physics - Experiment · Physics 2010-04-08 P. Rubin , CLEO Collaboration

We review some recent progress in understanding various exclusive double charmonium production processes at $B$ factories, within the nonrelativistic QCD factorization framework. First we investigate the impact of the joint perturbative and…

High Energy Physics - Phenomenology · Physics 2013-02-21 Hai-Rong Dong , Feng Feng , Yu Jia

We point out some properties of the amplitude of the dipion transition $\Upsilon(3S) \to \Upsilon(1S) \pi \pi$ in relation to the recently reported results of a CLEO analysis of form factors in this amplitude. We find that the reported…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Dubynskiy , M. B. Voloshin

Using data taken with the CLEO III detector, 1.09 fb-1 at Upsilon(1S), and 1.28 fb-1 at Upsilon(2S), branching fractions have been measured for the first time for exclusive decays of each resonance into one hundred different final states…

High Energy Physics - Experiment · Physics 2015-06-05 S. Dobbs , Z. Metreveli , A. Tomaradze , T. Xiao , Kamal K. Seth

We discuss the possibility that production of final states with bottomonium and light mesons at the peak $\Upsilon(6S)$ in the $e^+e^-$ annihilation at approximately 11.00 GeV is in fact due to a triangular singularity at the threshold of…

High Energy Physics - Phenomenology · Physics 2016-05-18 A. E. Bondar , M. B. Voloshin

Based on data collected by the CLEO III detector at CESR, we started a series of investigations to open the mysteries of the $\Upsilon$(5S) resonance decay properties. $B_s$ mesons are expected to decay predominantly into $D_s$ meson, while…

High Energy Physics - Experiment · Physics 2019-08-14 R. Sia