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Related papers: Recent CLEO Upsilon(1S) and Upsilon(3S) Results

200 papers

The $\Upsilon(1S+2S+3S)\to e^{+}e^{-}$ cross section is measured at mid-rapidity ($y$) in $p+p$ collisions and in d$+Au$ collisions at center-of-mass energy $\sqrt{s}$ = 200 GeV with the STAR detector at RHIC. In $p+p$, the measured cross…

Nuclear Experiment · Physics 2010-05-25 A. M. Hamed

Charged lepton flavour violating processes are unobservable in the standard model, but they are predicted to be enhanced in several new physics extensions. We present the results of a search for $\Upsilon (2S)$ and $\Upsilon (3S)$ decays to…

High Energy Physics - Experiment · Physics 2026-03-09 H. Ahmed , N. Tasneem , J. M. Roney

A search for the decays of the Higgs and $Z$ bosons to $J/\psi\gamma$ and $\Upsilon(nS)\gamma$ ($n=1,2,3$) is performed with $pp$ collision data samples corresponding to integrated luminosities of up to $20.3\mathrm{fb}^{-1}$ collected at…

High Energy Physics - Experiment · Physics 2015-04-01 ATLAS Collaboration

Using data collected in the Belle experiment at the KEKB asymmetric-energy $e^+e^-$ collider we search for transitions $\Upsilon(4S) \rightarrow \eta_b(1S)\omega$, $\Upsilon(5S) \rightarrow \eta_b(1S)\omega$ and $\Upsilon(5S) \rightarrow…

High Energy Physics - Experiment · Physics 2020-09-25 Belle Collaboration , P. Oskin , R. Mizuk , H. Aihara , D. M. Asner , H. Atmacan , V. Aulchenko , T. Aushev , R. Ayad , P. Behera , K. Belous , J. Bennett , M. Bessner , V. Bhardwaj , B. Bhuyan , T. Bilka , J. Biswal , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , M. Campajola , L. Cao , D. Červenkov , P. Chang , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , G. De Nardo , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , S. Dubey , S. Eidelman , D. Epifanov , T. Ferber , D. Ferlewicz , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , A. Giri , P. Goldenzweig , B. Golob , K. Gudkova , C. Hadjivasiliou , T. Hara , O. Hartbrich , H. Hayashii , M. T. Hedges , M. Hernandez Villanueva , W. -S. Hou , C. -L. Hsu , T. Iijima , K. Inami , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , S. Jia , Y. Jin , C. W. Joo , K. K. Joo , A. B. Kaliyar , K. H. Kang , G. Karyan , H. Kichimi , C. Kiesling , C. H. Kim , D. Y. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , S. Korpar , D. Kotchetkov , P. Križan , R. Kroeger , P. Krokovny , R. Kulasiri , R. Kumar , K. Kumara , Y. -J. Kwon , J. S. Lange , S. C. Lee , P. Lewis , C. H. Li , L. K. Li , L. Li Gioi , J. Libby , K. Lieret , D. Liventsev , M. Masuda , T. Matsuda , M. Merola , F. Metzner , K. Miyabayashi , H. Miyata , G. B. Mohanty , S. Mohanty , T. J. Moon , T. Mori , R. Mussa , M. Nakao , H. Nakazawa , A. Natochii , L. Nayak , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , K. Ogawa , S. Ogawa , H. Ono , Y. Onuki , P. Pakhlov , G. Pakhlova , T. Pang , S. Pardi , H. Park , S. -H. Park , S. Paul , R. Pestotnik , L. E. Piilonen , T. Podobnik , V. Popov , E. Prencipe , M. T. Prim , A. Rostomyan , N. Rout , G. Russo , D. Sahoo , Y. Sakai , A. Sangal , L. Santelj , T. Sanuki , V. Savinov , G. Schnell , J. Schueler , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , M. Shapkin , C. P. Shen , J. -G. Shiu , A. Sokolov , E. Solovieva , M. Starič , Z. S. Stottler , K. Sumisawa , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , K. Trabelsi , T. Uglov , Y. Unno , S. Uno , Y. Usov , S. E. Vahsen , R. Van Tonder , G. Varner , A. Vinokurova , V. Vorobyev , E. Waheed , C. H. Wang , E. Wang , M. -Z. Wang , P. Wang , M. Watanabe , S. Watanuki , S. Wehle , J. Wiechczynski , E. Won , X. Xu , B. D. Yabsley , W. Yan , S. B. Yang , H. Ye , J. Yelton , J. H. Yin , C. Z. Yuan , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhukova

Using CLEO data, we study the production of the anti-deuteron, d-bar, in Upsilon(nS) resonance decays and the nearby continuum. The branching ratios obtained are B^dir(Upsilon(1S) --> d-bar X) = (3.36 +- 0.23 +- 0.25) x 10^-5, B(Upsilon(1S)…

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

In this work, we investigate the characteristics of the spin-singlet state $\eta_b$ of the bottomonia family via the radiative decays of $\Upsilon(nS)\to \eta_b+\gamma$. The theoretical estimation of the decay widths is carried out in terms…

High Energy Physics - Phenomenology · Physics 2010-03-01 Hong-Wei Ke , Xue-Qian Li , Xiang Liu

We measure the production cross sections for e+e- -> Upsilon(1S)pi+pi-, Upsilon(2S)pi+pi-, and Upsilon(3S)pi+pi- as a function of sqrt{s} between 10.83 GeV and 11.02 GeV. The data consists of 8.1 fb^-1 collected with the Belle detector at…

High Energy Physics - Experiment · Physics 2013-05-29 The Belle Collaboration , K. -F. Chen , W. -S. Hou

The angular distributions of Upsilon(1S) to mu+ mu- decays are analyzed using a sample of Upsilon(1S) mesons in 2.9 fb^{-1} of data collected at sqrt{s} = 1.96TeV. The results of the one-dimensional angular analysis suggest that Upsilon(1S)…

High Energy Physics - Experiment · Physics 2011-10-04 Niharika Ranjan

We report on the status of a variety of radiative B decays studied by the CLEO detector with $9.7\times 10^6$ $B\bar{B}$ pairs.

High Energy Physics - Phenomenology · Physics 2007-05-23 T. E. Coan

Using the data samples of 102 million $\Upsilon(1S)$ and 158 million $\Upsilon(2S)$ events collected by the Belle detector, we search for a pentaquark state in the $pJ/\psi$ final state from $\Upsilon(1,2S)$ inclusive decays. Here, the…

High Energy Physics - Experiment · Physics 2025-08-11 Belle Collaboration , X. Dong , S. M. Zou , H. Y. Zhang , X. L. Wang , I. Adachi , J. K. Ahn , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , R. Ayad , S. Bahinipati , Sw. Banerjee , M. Bessner , V. Bhardwaj , D. Biswas , D. Bodrov , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , D. Červenkov , M. -C. Chang , P. Chang , B. G. Cheon , H. E. Cho , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , S. Das , G. De Nardo , G. De Pietro , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , P. Ecker , D. Epifanov , T. Ferber , D. Ferlewicz , B. G. Fulsom , R. Garg , V. Gaur , A. Giri , P. Goldenzweig , E. Graziani , T. Gu , Y. Guan , K. Gudkova , C. Hadjivasiliou , H. Hayashii , S. Hazra , M. T. Hedges , W. -S. Hou , C. -L. Hsu , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , S. Jia , Y. Jin , D. Kalita , T. Kawasaki , D. Y. Kim , K. -H. Kim , Y. J. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , P. Krokovny , T. Kuhr , R. Kumar , T. Kumita , A. Kuzmin , Y. -J. Kwon , Y. -T. Lai , T. Lam , J. S. Lange , D. Levit , L. K. Li , Y. Li , Y. B. Li , L. Li Gioi , J. Libby , D. Liventsev , Y. Ma , M. Masuda , T. Matsuda , S. K. Maurya , F. Meier , M. Merola , F. Metzner , K. Miyabayashi , R. Mussa , I. Nakamura , T. Nakano , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , S. Nishida , S. Ogawa , H. Ono , G. Pakhlova , S. Pardi , H. Park , J. Park , S. -H. Park , A. Passeri , S. Patra , S. Paul , 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 , J. B. Singh , E. Solovieva , M. Starič , M. Takizawa , K. Tanida , F. Tenchini , R. Tiwary , M. Uchida , Y. Unno , S. Uno , P. Urquijo , Y. Usov , A. Vinokurova , S. Watanuki , E. Won , B. D. Yabsley , W. Yan , S. B. Yang , J. Yelton , J. H. Yin , Y. Yook , C. Z. Yuan , L. Yuan , Y. Yusa , Z. P. Zhang , V. Zhilich

The dielectron widths of $\Upsilon(nS) (n=1,...,7)$ and vector decay constants are calculated using the Relativistic String Hamiltonian with a universal interaction. For $\Upsilon(nS) (n=1,2,3)$ the dielectron widths and their ratios are…

High Energy Physics - Phenomenology · Physics 2010-02-17 A. M. Badalian , B. L. G. Bakker , I. V. Danilkin

We perform the investigation of two-body hidden-bottom transitions of the $\Upsilon(6S)$, which include $\Upsilon(6S) \to \Upsilon(1^3D_J) \eta~~(J=1,2,3)$ decays. For estimating the branching ratios of these processes, we consider…

High Energy Physics - Phenomenology · Physics 2018-05-22 Qi Huang , Hao Xu , Xiang Liu , Takayuki Matsuki

We report the initial results from CLEO-c based on the 55.8/pb data obtained at the psi(3770) resonance last year. We give a concise summary of the various CLEO-c analyses on leptonic and semileptonic decays of neutral and charged D mesons.…

High Energy Physics - Experiment · Physics 2019-08-14 Doris Yangsoo Kim

The CMS collaboration has reported a measurement of $\Upsilon$ decays to ditaus using $61.9~{\rm fb}^{-1}$ of scouting data. If interpreted as the decay of $\Upsilon(1S,2S,3S)$, the measured ditau rate is more than ten times that seen in…

High Energy Physics - Phenomenology · Physics 2026-05-29 Matthew R Buckley , David Shih , Isaac R Wang

In this work, we propose a possible experimental research topic on the $\Upsilon(6S)\to \Upsilon(nS)\eta^{(\prime)}$ ($n=1,2,3$) transitions. Considering the hadronic loop effect from the intermediate $S$-wave $B_{(s)}$ and $B_{(s)}^*$…

High Energy Physics - Phenomenology · Physics 2018-09-12 Qi Huang , Xiang Liu , Takayuki Matsuki

We study the Upsilon(3S,2S)->eta Upsilon(1S) and Upsilon(3S,2S)->pi+pi- Upsilon(1S) transitions with 122 million Upsilon(3S) and 100 million Upsilon(2S) mesons collected by the BaBar detector at the PEP-II asymmetric energy e+e- collider.…

High Energy Physics - Experiment · Physics 2013-05-29 The BABAR Collaboration , J. P. Lees , others

Using a sample of 3.3 million Upsilon(4S) -> BBbar events collected with the CLEO II detector at the Cornell Electron Storage Ring (CESR), we measure the branching fraction for B -> rho l nu, |V_ub|, and the partial rate (Delta Gamma) in…

High Energy Physics - Experiment · Physics 2010-04-08 B. H. Behrens

Using the CLEO detector at the Cornell Electron Storage Ring, we have observed the Bs meson in e+e- annihilation at the Upsilon(5S) resonance. We find 14 candidates consistent with Bs decays into final states with a J/psi or a Ds(*)-. The…

High Energy Physics - Experiment · Physics 2010-04-08 G. Bonvicini , CLEO Collaboration

The CLEO detector will undergo major improvements in conjunction with a high luminosity upgrade of the CESR electron positron collider, that should increase the luminosity of this machine by a factor of 10. The most innovative feature of…

High Energy Physics - Experiment · Physics 2008-11-26 Marina Artuso

We study hadronic transitions between bottomonium states using 496 fb$^{-1}$ data collected at the $\Upsilon(4S)$ resonance with the Belle detector at the KEKB asymmetric energy $e^{+}e^{-}$ collider. We measure: ${\cal…

High Energy Physics - Experiment · Physics 2017-10-04 Belle Collaboration , E. Guido , R. Mussa , U. Tamponi , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , V. Aulchenko , T. Aushev , R. Ayad , I. Badhrees , A. M. Bakich , V. Bansal , P. Behera , V. Bhardwaj , B. Bhuyan , J. Biswal , A. Bobrov , A. Bondar , A. Bozek , M. Bračko , T. E. Browder , D. Červenkov , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , K. Cho , S. -K. Choi , Y. Choi , D. Cinabro , N. Dash , S. Di Carlo , Z. Doležal , Z. Drásal , S. Eidelman , D. Epifanov , H. Farhat , J. E. Fast , T. Ferber , B. G. Fulsom , V. Gaur , N. Gabyshev , A. Garmash , M. Gelb , R. Gillard , P. Goldenzweig , J. Haba , T. Hara , K. Hayasaka , H. Hayashii , M. T. Hedges , W. -S. Hou , T. Iijima , K. Inami , G. Inguglia , A. Ishikawa , R. Itoh , Y. Iwasaki , W. W. Jacobs , I. Jaegle , H. B. Jeon , S. Jia , Y. Jin , D. Joffe , K. K. Joo , T. Julius , K. H. Kang , G. Karyan , T. Kawasaki , D. Y. Kim , J. B. Kim , K. T. Kim , M. J. Kim , S. H. Kim , Y. J. Kim , K. Kinoshita , P. Kodyš , S. Korpar , D. Kotchetkov , P. Križan , P. Krokovny , R. Kulasiri , T. Kumita , A. Kuzmin , Y. -J. Kwon , J. S. Lange , P. Lewis , C. H. Li , L. Li , L. Li Gioi , J. Libby , D. Liventsev , M. Lubej , T. Luo , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , K. Miyabayashi , H. Miyata , R. Mizuk , H. K. Moon , T. Mori , E. Nakano , M. Nakao , T. Nanut , K. J. Nath , Z. Natkaniec , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , S. Ogawa , H. Ono , P. Pakhlov , G. Pakhlova , B. Pal , S. Pardi , C. -S. Park , H. Park , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , C. Pulvermacher , M. Ritter , A. Rostomyan , Y. Sakai , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , V. Shebalin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , F. Simon , A. Sokolov , E. Solovieva , M. Starič , J. F. Strube , K. Sumisawa , T. Sumiyoshi , M. Takizawa , K. Tanida , F. Tenchini , K. Trabelsi , M. Uchida , T. Uglov , Y. Unno , S. Uno , Y. Usov , C. Van Hulse , G. Varner , A. Vinokurova , V. Vorobyev , A. Vossen , C. H. Wang , P. Wang , M. Watanabe , Y. Watanabe , S. Watanuki , E. Widmann , K. M. Williams , E. Won , Y. Yamashita , H. Ye , C. Z. Yuan , Z. P. Zhang , V. Zhukova , V. Zhulanov , A. Zupanc
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