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We report a measurement of the production ratio of charged and neutral B mesons from Upsilon(4S) decays based on the ratio of efficiency-corrected yields for the charmonium modes J/psi K^+ and J/psi K^{0}_{S} with 81.9 fb^-1 of data…

High Energy Physics - Experiment · Physics 2008-11-26 B. Aubert , BABAR Collaboration

We analyze 9.7 x 10^6 B\bar{B}$ pairs recorded with the CLEO detector to determine the production ratio of charged to neutral B-meson pairs produced at the Y(4S) resonance. We measure the rates for B^0 -> J/psi K^{(*)0} and B^+ -> J/psi…

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

This paper presents a detailed description of a model-independent method for the direct measurement of the $\Upsilon(4S) \to B^+ B^-$ and $\Upsilon(4S) \to B^0 \bar{B}^0$ production fractions at $B$ factories. The method is based on…

High Energy Physics - Phenomenology · Physics 2026-04-03 Murad Yasaveev , Pavel Pakhlov , Nikolai Peters , Alena Mufazalova

The ratio of charged and neutral B meson production at the Upsilon(4S), f_{+-}/f_{00}, is measured through the decays B bar -> D* l- nu_l bar, reconstructed using a partial reconstruction method where the D* is detected only through a pion…

High Energy Physics - Experiment · Physics 2010-04-08 S. B. Athar , CLEO Collaboration

Using 420 pb^-1 of data collected on the Upsilon(5S) resonance with the CLEO III detector, we reconstruct B mesons in 25 exclusive decay channels to measure or set upper limits on the decay rate of Upsilon(5S) into B meson final states. We…

High Energy Physics - Experiment · Physics 2010-04-08 O. Aquines , CLEO Collaboration

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

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 introduce a new method for the determination of the ratio of production fractions $R^{\pm0}=\mathcal B(\Upsilon(4S)\to B^+B^-)/\mathcal B(\Upsilon(4S)\to B^0\bar B^0)$ based on $\bar B\to D^{(*)}\ell\bar \nu$ decays. Given the importance…

High Energy Physics - Phenomenology · Physics 2026-04-10 Martin Jung , Stefan Schacht

The $B$ factories are expected to provide huge samples of single $B$ decay events with little background by reconstructing one of the $B$ mesons produced in $\Upsilon (4S)$ decays. This represents a new experimental paradigm: such samples…

High Energy Physics - Phenomenology · Physics 2011-09-13 I. I. Bigi

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

We report a measurement of the $B^0-\bar{B}^0$ mixing parameter $\Delta m_d$ based on a $\rm 29.1~fb^{-1}$ sample of $\Upsilon (4S)$ resonance decays collected by the Belle detector at the KEKB asymmetric $e^+ e^-$ collider. We use events…

High Energy Physics - Experiment · Physics 2010-03-26 Y. Zheng , T. E. Browder

Knowledge of the Bs decay fraction of the Y(5S) resonance, fs, is important for Bs meson studies at the Y(5S) energy. Using data collected by the CLEO III detector at CESR consisting of 0.423 1/fb on the Y(5S) resonance, 6.34 1/fb on the…

High Energy Physics - Experiment · Physics 2007-05-23 G. Huang , CLEO Collaboration

The large data sample being recorded with the Belle detector at the $\Upsilon$(5S) energy provides a unique opportunity to study the less-well-known $B_s^{0}$ meson decays. Following our recent measurement of $B_s^{0}\to D_s^{-}\pi^{+}$ in…

High Energy Physics - Experiment · Physics 2019-08-13 Sevda Esen

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

Methods are proposed for measuring the ratio $R^{+/0} = \Gamma(\Upsilon(4S) \to B^+ B^-)/$ $\Gamma(\Upsilon(4S) \to \bo \ob)$ without assuming isospin invariance in exclusive hadronic decays such as $B \to J/\psi K$. The validity of isospin…

High Energy Physics - Phenomenology · Physics 2008-11-26 Michael Gronau , Yuval Grossman , Jonathan L. Rosner

Decays of the Y(5S) resonance to channels with B^+ and B^0 mesons are studied using a 23.6 fb^{-1} data sample collected with the Belle detector at the KEKB asymmetric-energy e^+ e^- collider. Fully reconstructed B^+ -> J/\psi K^+, B^0 ->…

High Energy Physics - Experiment · Physics 2019-08-13 A. Drutskoy

BaBar experiment scan around the Upsilon(4S) resonance and measure its mass and full width. They also measure Br(Upsilon(4S) -> B0 B0b) = 0.486 +/- 0.010 +/- 0.009 from 81.7 fb-1 Upsilon(4S) data. CLEO collaboration took about 0.42 fb-1…

High Energy Physics - Experiment · Physics 2017-08-23 J. C. Wang

Recent rate measurements of B_s mesons and Lambda_b baryons produced in sqrt{s} = 1.96 TeV proton-antiproton and Upsilon(5S) electron-positron collisions are reviewed, including the first observations of six new decay modes: B_s -> D_s^+…

High Energy Physics - Experiment · Physics 2012-11-14 Andreas Warburton

We present the first measurement of $\Upsilon(4S)$ decays to $\pi^+pi^-\Upsilon(1S)$ and $\pi^+pi^-\Upsilon(2S)$ based on a sample of 230$\times10^6$ $\Upsilon(4S)$ mesons collected with the BABAR detector. We measure the product branching…

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

Theoretical predictions for B decay rates are rewritten in terms of the Upsilon meson mass instead of the b quark mass, using a modified perturbation expansion. The theoretical consistency is shown both at low and high orders. This method…

High Energy Physics - Phenomenology · Physics 2007-05-23 Zoltan Ligeti
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