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Related papers: Study of the ${\Upsilon}(1S)$ ${\to}$ $DP$ decays

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Analyzing $\Upsilon(nS)$ decays acquired with the CLEO detector operating at the CESR $e^+e^-$ collider, we measure for the first time the product branching fractions ${\cal B}[\Upsilon(nS)\to\gamma\chi_{b}((n-1)P_J)] \times {\cal…

High Energy Physics - Experiment · Physics 2010-04-08 CLEO Collaboration , D. M. Asner

A calculation is presented of the radiative decay of the Upsilon(nS) into a bound state of bottom squarks. Predictions are provided of the branching fraction as a function of the masses of the bottom squark and the gluino. Branching…

High Energy Physics - Phenomenology · Physics 2008-11-26 Edmond L. Berger , Geoffrey T. Bodwin , Jungil Lee

Motivated by the recent measurement of the upper limit of ${B}^0 \to J/\psi D$ branching ratio, which is important in accounting for the soft $J/\psi$ production in B decays, we investigate ${B}^0 \to J/\psi D^{(\star)}$ and $\eta_c…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ying Li , Cai-Dian Lu , Cong-Feng Qiao

We report on a study of exclusive radiative decays of the Upsilon(1S) resonance collected with the CLEO-II detector operating at CESR. We present the first observation of the radiative decays Upsilon(1S)->gamma pi+pi- and Upsilon(1S)->gamma…

High Energy Physics - Experiment · Physics 2010-04-08 A. Anastassov

We have searched for the decays $B^0 \rightarrow D_s^{+}a_0^-$, $B^0 \rightarrow D_s^{*+}a_0^-$, $B^0 \rightarrow D_s^{+}a_2^-$ and $B^0 \rightarrow D_s^{*+}a_2^-$ in a sample of about 230 million $\Upsilon(4S) \rightarrow B{\bar B}$ decays…

High Energy Physics - Experiment · Physics 2010-03-19 The BABAR Collaboration , B. Aubert et al

We investigate the $B \to K^{*}\pi$ decays, one of hardly understandable processes among charmless B-meson decays, within the perturbative QCD method. Owing to the dynamically enhanced mechanism in PQCD, we obtain large branching ratios and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Y. -Y. Keum

We study inclusive di-pion decays using a sample of 108 x 10^6 Upsilon(3S) events recorded with the BABAR detector. We search for the decay mode Upsilon(3S) --> pi+ pi- h_b(1P) and find no evidence for the bottomonium spin-singlet state…

High Energy Physics - Experiment · Physics 2012-08-27 The BABAR Collaboration

In this study we present the first theoretical calculation of the form factor of the $\chi_{c0}(1P) \rar J/\psi \gamma $ and $\chi_{b0}(1P) \rightarrow \Upsilon(1S) \gamma $ decays in the frame work of QCD sum rules. We also find branching…

High Energy Physics - Phenomenology · Physics 2013-05-29 v. Bashiry

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

Two body $B$ meson decays involving the radially excited meson $\psi(2S)/\eta_c(2S)$ in the final states are studied by using the perturbative QCD (pQCD) approach. We find that: (a) The branching ratios for the decays involving $K$ meson…

High Energy Physics - Phenomenology · Physics 2017-10-11 Zhi-Qing Zhang

In the work, we study the production of dark baryon $\psi$ with the bottom-baryon decays $\Lambda_b\to M \psi$ under the perturbative QCD approach. For the Type-I/II models in B-Mesogenesis scenarios, we calculate the form factors for…

High Energy Physics - Phenomenology · Physics 2025-08-08 Ye Xing , Yu-Ji Shi , Xiao-Hui Hu

We study the rare hadronic transitions $\Upsilon(2S)\rightarrow \Upsilon(1S)\eta$ and $\Upsilon(2S)\rightarrow \Upsilon(1S)\pi^0$ using a sample of 158 $\times 10^6$ $\Upsilon(2S)$ decays collected with the Belle detector at the KEKB…

High Energy Physics - Experiment · Physics 2013-05-30 Belle Collaboration , U. Tamponi , R. Mussa , I. Adachi , H. Aihara , D. M. Asner , V. Aulchenko , T. Aushev , A. M. Bakich , M. Barrett , B. Bhuyan , A. Bondar , A. Bozek , M. Bra\v , T. E. Browder , A. Chen , P. Chen , B. G. Cheon , K. Chilikin , I. -S. Cho , K. Cho , Y. Choi , J. Dalseno , Z. Dole\v , Z. Drásal , D. Dutta , S. Eidelman , D. Epifanov , S. Esen , H. Farhat , J. E. Fast , A. Frey , V. Gaur , R. Gillard , Y. M. Goh , B. Golob , K. Hayasaka , Y. Horii , Y. Hoshi , H. J. Hyun , T. Iijima , A. Ishikawa , Y. Iwasaki , I. Jaegle , J. H. Kang , T. Kawasaki , H. O. Kim , J. H. Kim , K. T. Kim , M. J. Kim , Y. J. Kim , J. Klucar , B. R. Ko , P. Kody\v , S. Korpar , R. T. Kouzes , P. Kri\v , P. Krokovny , T. Kumita , A. Kuzmin , S. -H. Lee , Y. Li , C. Liu , Y. Liu , Z. Q. Liu , D. Liventsev , H. Miyata , R. Mizuk , G. B. Mohanty , A. Moll , N. Muramatsu , M. Nakao , Z. Natkaniec , C. Ng , S. Nishida , O. Nitoh , S. Ogawa , T. Ohshima , S. Okuno , S. L. Olsen , Y. Onuki , P. Pakhlov , H. K. Park , K. S. Park , T. K. Pedlar , R. Pestotnik , M. Petri\v , L. E. Piilonen , M. Röhrken , Y. Sakai , S. Sandilya , D. Santel , L. Santelj , T. Sanuki , O. Schneider , G. Schnell , C. Schwanda , K. Senyo , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , F. Simon , P. Smerkol , Y. -S. Sohn , A. Sokolov , E. Solovieva , M. Stari\v , T. Sumiyoshi , K. Tanida , N. Taniguchi , G. Tatishvili , Y. Teramoto , K. Trabelsi , S. Uehara , S. Uno , C. Van Hulse , P. Vanhoefer , G. Varner , C. H. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , K. M. Williams , E. Won , B. D. Yabsley , Y. Yamashita , C. Z. Yuan , Z. P. Zhang , V. Zhilich , V. Zhulanov , A. Zupanc

In this work, we investigate the $\Upsilon(10753)\to\Upsilon(nS)\pi^+\pi^-$ ($n=1,2,3$) processes by considering the hadronic loop mechanism, where $\Upsilon(10753)$ is assigned to a conventional bottomonium in the $4S$-$3D$ mixing scheme.…

High Energy Physics - Phenomenology · Physics 2022-04-19 Zi-Yue Bai , Yu-Shuai Li , Qi Huang , Xiang Liu , Takayuki Matsuki

In this short presentation I emphasize the increased importance of kaon flavour physics in the search for new physics (NP) that we should witness in the rest of this decade and in the next decade. The main actors will be the branching…

High Energy Physics - Phenomenology · Physics 2017-04-05 Andrzej J. Buras

An elegant and more precise formula for the 3-loop perturbative QCD coupling is discussed. It improves the common expression (e.g., canonized by PDG) in few GeV region. On its base, we propose simple analytic Model for ghost-free QCD…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. V. Shirkov

In the framework of the perturbative QCD approach, we study the charmless pure weak annihilation Bc->KK decay and find that the branching ratio BR(Bc->KK) O(10^-7). This prediction is so tiny that the Bc->KK decay might be unmeasurable at…

High Energy Physics - Phenomenology · Physics 2011-11-10 Yue-Ling Yang , Jun-Feng Sun , Na Wang

The decay psi(2S)-->K_S K_L is observed for the first time using psi(2S) data collected with the Beijing Spectrometer (BESII) at the Beijing Electron Positron Collider (BEPC); the branching ratio is determined to be B(psi(2S)-->K_S K_L) =…

High Energy Physics - Experiment · Physics 2019-08-14 J. Z. Bai

The decays of $\jpsi$ and $\psip$ to ${n}{K^0_S}\bar{\Lambda}+c.c.$ are observed and measured for the first time, and the perturbative QCD ``12%'' rule is tested, based on $5.8 \times 10^7$ $\jpsi$ and $1.4 \times 10^7$ $\psip$ events…

High Energy Physics - Experiment · Physics 2012-08-27 BES Collaboration

The rare decays $B^0 \to D_s^- K^+$ and $B^+ \to D_s^+ \bar{K}^0$ can occur only via annihilation type diagrams in the standard model. We calculate these decays in perturbative QCD approach. We found that the calculated branching ratio of…

High Energy Physics - Phenomenology · Physics 2009-01-07 Cai-Dian Lu , Kazumasa Ukai

To clarify the conflict between the theoretical predictions and experimental measurements of the inclusive J/psi production in Upsilon decay, We consider the alpha_s^6 order color-singlet contributions of processes Upsilon --> J/psi+gg and…

High Energy Physics - Phenomenology · Physics 2010-12-23 Zhi-Guo He , Jian-Xiong Wang
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