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Related papers: Upsilon Decays at CLEO

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The di-electron width of an Upsilon meson is the decay rate of the Upsilon into an electron-positron pair, expressed in units of energy. We measure the di-electron width of the Upsilon(1S) meson to be 1.354 +- 0.004 +- 0.020 keV (the first…

High Energy Physics - Experiment · Physics 2011-11-09 J. Pivarski

We present an improved measurement of the $\eta'$ meson energy spectrum in $\Upsilon(1S)$ decays, using 1.2 fb^{-1} of data taken at the $\Upsilon(1S)$ center-of-mass energy with the CLEO III detector. We compare our results with models of…

High Energy Physics - Experiment · Physics 2014-11-17 O. Aquines , CLEO Collaboration

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

Using a data sample collected with the CLEO II detector at CESR, we have searched for dipion transitions between pairs of $\Upsilon$ resonances at energies near the $\Upsilon(4S)$. We obtain upper limits $B(\Upsilon(4S)\to…

High Energy Physics - Experiment · Physics 2010-04-08 S. Glenn

Using 5.46 pb$^{-1}$ of $e^+e^-$ annihilation data collected at the $\psi(2S)$ with the CLEO detector we have observed a variety of new hadronic decay modes of the $\psi(2S)$. A comprehensive set of branching ratios and upper limits is…

High Energy Physics - Experiment · Physics 2019-08-14 G. S. Huang

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

We report results of a search for the invisible decay of the Upsilon(1S) via the Upsilon(3S)->pi+pi-Upsilon(1S) transition using a data sample of 2.9 fb^{-1} at the Upsilon(3S) resonance. The data were collected with the Belle detector at…

High Energy Physics - Experiment · Physics 2008-11-26 The Belle Collaboration , O. Tajima , H. Hayashii , M. Hazumi , K. Inami , Y. Iwasaki , S. Uehara

Heavy Quarkonium Physics continues to be a focus of the work done by the CLEO Collaboration. We present several results in the spectroscopy of both bottomonium and charmonium systems using CLEO's data sets taken at the Upsilon(3S),…

High Energy Physics - Experiment · Physics 2019-08-13 T. K. Pedlar

Using 9.32, 5.88 million Upsilon(2S,3S) decays taken with the CLEO-III detector, we obtain five product branching fractions for the exclusive processes Upsilon(2S) => gamma chi_{b0,1,2}(1P) => gamma gamma Upsilon(1S) and Upsilon(3S) =>…

We present an improved measurement of the eta' meson energy spectrum in Upsilon(1S) decays, using 1.2 fb^{-1}} of data taken at the Upsilon(1S) center-of-mass energy with the CLEO III detector. We compare our results with models of eta'…

High Energy Physics - Experiment · Physics 2007-05-23 O. Aquines , CLEO Collaboration

We report on a search for the radiative decay of Upsilon(1S) to the pseudoscalar mesons eta and etaprime in 21.2 +/- 0.2 times 10^6 Upsilon(1S) decays collected with the CLEO III detector at the Cornell Electron Storage Ring (CESR). The eta…

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

We have studied the leptonic decay of the $\Upsilon (1S)$ resonance into tau pairs using the CLEO II detector. A clean sample of tau pair events is identified via events containing two charged particles where exactly one of the particles is…

High Energy Physics - Experiment · Physics 2009-09-25 D. Cinabro

Using data taken with the CLEO III detector at the Cornell Electron Storage Ring, we have investigated the direct photon spectrum in the decays Upsilon(1S) -> gggamma, Upsilon(2S) -> gggamma, Upsilon}(3S) -> gggamma. The latter two of these…

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

Using a data sample of $\Upsilon(2S)$ events collected with the CLEO II detector at the Cornell Electron Storage Ring, we have investigated the hadronic transitions between the $\Upsilon(2S)$ and the $\Upsilon(1S)$. The charged dipion…

High Energy Physics - Experiment · Physics 2010-04-08 J. Alexander

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 report a study of radiative decays of \chi_{bJ}(1P)(J=0,1,2) mesons into 74 hadronic final states comprising charged and neutral pions, kaons, protons; out of these, 41 modes are observed with at least 5 standard deviation significance.…

High Energy Physics - Experiment · Physics 2016-08-06 A. Abdesselam , I. Adachi , K. Adamczyk , H. Aihara , S. Al Said , K. Arinstein , Y. Arita , D. M. Asner , T. Aso , H. Atmacan , V. Aulchenko , T. Aushev , R. Ayad , T. Aziz , V. Babu , I. Badhrees , S. Bahinipati , A. M. Bakich , A. Bala , Y. Ban , V. Bansal , E. Barberio , M. Barrett , W. Bartel , A. Bay , I. Bedny , P. Behera , M. Belhorn , K. Belous , M. Berger , D. Besson , V. Bhardwaj , B. Bhuyan , J. Biswal , T. Bloomfield , S. Blyth , A. Bobrov , A. Bondar , G. Bonvicini , C. Bookwalter , C. Boulahouache , A. Bozek , M. Bračko , F. Breibeck , J. Brodzicka , T. E. Browder , E. Waheed , D. Červenkov , M. -C. Chang , P. Chang , Y. Chao , V. Chekelian , A. Chen , K. -F. Chen , P. Chen , B. G. Cheon , K. Chilikin , R. Chistov , K. Cho , V. Chobanova , S. -K. Choi , Y. Choi , D. Cinabro , J. Crnkovic , J. Dalseno , M. Danilov , N. Dash , S. Di Carlo , J. Dingfelder , Z. Doležal , D. Dossett , Z. Drásal , A. Drutskoy , S. Dubey , D. Dutta , K. Dutta , S. Eidelman , D. Epifanov , S. Esen , H. Farhat , J. E. Fast , M. Feindt , T. Ferber , A. Frey , O. Frost , B. G. Fulsom , V. Gaur , N. Gabyshev , S. Ganguly , A. Garmash , D. Getzkow , R. Gillard , F. Giordano , R. Glattauer , Y. M. Goh , P. Goldenzweig , B. Golob , D. Greenwald , M. Grosse Perdekamp , J. Grygier , O. Grzymkowska , H. Guo , J. Haba , P. Hamer , Y. L. Han , K. Hara , T. Hara , Y. Hasegawa , J. Hasenbusch , K. Hayasaka , H. Hayashii , X. H. He , M. Heck , M. T. Hedges , D. Heffernan , M. Heider , A. Heller , T. Higuchi , S. Himori , S. Hirose , T. Horiguchi , Y. Hoshi , K. Hoshina , W. -S. Hou , Y. B. Hsiung , C. -L. Hsu , M. Huschle , H. J. Hyun , Y. Igarashi , T. Iijima , M. Imamura , K. Inami , G. Inguglia , A. Ishikawa , K. Itagaki , R. Itoh , M. Iwabuchi , M. Iwasaki , Y. Iwasaki , S. Iwata , W. W. Jacobs , I. Jaegle , H. B. Jeon , D. Joffe , M. Jones , K. K. Joo , T. Julius , H. Kakuno , J. H. Kang , K. H. Kang , P. Kapusta , S. U. Kataoka , E. Kato , Y. Kato , P. Katrenko , H. Kawai , T. Kawasaki , T. Keck , H. Kichimi , C. Kiesling , B. H. Kim , D. Y. Kim , H. J. Kim , H. -J. Kim , J. B. Kim , J. H. Kim , K. T. Kim , M. J. Kim , S. H. Kim , S. K. Kim , Y. J. Kim , K. Kinoshita , C. Kleinwort , J. Klucar , B. R. Ko , N. Kobayashi , S. Koblitz , P. Kodyš , Y. Koga , S. Korpar , D. Kotchetkov , R. T. Kouzes , P. Križan , P. Krokovny , B. Kronenbitter , T. Kuhr , L. Kulasiri , R. Kumar , T. Kumita , E. Kurihara , Y. Kuroki , A. Kuzmin , P. Kvasnička , Y. -J. Kwon , Y. -T. Lai , J. S. Lange , D. H. Lee , I. S. Lee , S. -H. Lee , M. Leitgab , R. Leitner , D. Levit , P. Lewis , C. H. Li , H. Li , J. Li , L. Li , X. Li , Y. Li , L. Li Gioi , J. Libby , A. Limosani , C. Liu , Y. Liu , Z. Q. Liu , D. Liventsev , A. Loos , R. Louvot , M. Lubej , P. Lukin , T. Luo , J. MacNaughton , M. Masuda , T. Matsuda , D. Matvienko , A. Matyja , S. McOnie , Y. Mikami , K. Miyabayashi , Y. Miyachi , H. Miyake , H. Miyata , Y. Miyazaki , R. Mizuk , G. B. Mohanty , S. Mohanty , D. Mohapatra , A. Moll , H. K. Moon , T. Mori , T. Morii , H. -G. Moser , T. Müller , N. Muramatsu , R. Mussa , T. Nagamine , Y. Nagasaka , Y. Nakahama , I. Nakamura , K. R. Nakamura , E. Nakano , H. Nakano , T. Nakano , M. Nakao , H. Nakayama , H. Nakazawa , T. Nanut , K. J. Nath , Z. Natkaniec , M. Nayak , E. Nedelkovska , K. Negishi , K. Neichi , C. Ng , C. Niebuhr , M. Niiyama , N. K. Nisar , S. Nishida , K. Nishimura , O. Nitoh , T. Nozaki , A. Ogawa , S. Ogawa , T. Ohshima , S. Okuno , S. L. Olsen , Y. Ono , Y. Onuki , W. Ostrowicz , C. Oswald , H. Ozaki , P. Pakhlov , G. Pakhlova , B. Pal , H. Palka , E. Panzenböck , C. -S. Park , C. W. Park , H. Park , K. S. Park , S. Paul , L. S. Peak , T. K. Pedlar , T. Peng , L. Pesántez , R. Pestotnik , M. Peters , M. Petrič , L. E. Piilonen , A. Poluektov , K. Prasanth , M. Prim , K. Prothmann , C. Pulvermacher , M. V. Purohit , J. Rauch , B. Reisert , E. Ribežl , M. Ritter , M. Röhrken , J. Rorie , A. Rostomyan , M. Rozanska , S. Rummel , S. Ryu , H. Sahoo , T. Saito , K. Sakai , Y. Sakai , S. Sandilya , D. Santel , L. Santelj , T. Sanuki , N. Sasao , Y. Sato , V. Savinov , T. Schlüter , O. Schneider , G. Schnell , P. Schönmeier , M. Schram , C. Schwanda , A. J. Schwartz , B. Schwenker , R. Seidl , Y. Seino , D. Semmler , K. Senyo , O. Seon , I. S. Seong , M. E. Sevior , L. Shang , M. Shapkin , V. Shebalin , C. P. Shen , T. -A. Shibata , H. Shibuya , S. Shinomiya , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , J. B. Singh , R. Sinha , P. Smerkol , Y. -S. Sohn , A. Sokolov , Y. Soloviev , E. Solovieva , S. Stanič , M. Starič , M. Steder , J. F. Strube , J. Stypula , S. Sugihara , A. Sugiyama , M. Sumihama , K. Sumisawa , T. Sumiyoshi , K. Suzuki , K. Suzuki , S. Suzuki , S. Y. Suzuki , Z. Suzuki , H. Takeichi , M. Takizawa , U. Tamponi , M. Tanaka , S. Tanaka , K. Tanida , N. Taniguchi , G. N. Taylor , F. Tenchini , Y. Teramoto , I. Tikhomirov , K. Trabelsi , V. Trusov , Y. F. Tse , T. Tsuboyama , M. Uchida , T. Uchida , S. Uehara , K. Ueno , T. Uglov , Y. Unno , S. Uno , S. Uozumi , P. Urquijo , Y. Ushiroda , Y. Usov , S. E. Vahsen , C. Van Hulse , P. Vanhoefer , G. Varner , K. E. Varvell , K. Vervink , A. Vinokurova , V. Vorobyev , A. Vossen , M. N. Wagner , E. Waheed , C. H. Wang , J. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , R. Wedd , S. Wehle , E. White , E. Widmann , J. Wiechczynski , K. M. Williams , E. Won , B. D. Yabsley , S. Yamada , H. Yamamoto , J. Yamaoka , Y. Yamashita , M. Yamauchi , S. Yashchenko , H. Ye , J. Yelton , Y. Yook , C. Z. Yuan , Y. Yusa , C. C. Zhang , L. M. Zhang , Z. P. Zhang , L. Zhao , V. Zhilich , V. Zhukova , V. Zhulanov , M. Ziegler , T. Zivko , A. Zupanc , N. Zwahlen , O. Zyukova

At CLEO, charmonium spectroscopy is pursued both thorugh e+e- annihilation data taken in the Upsilon region and more recently at psi(2S). A nmber of first observations (eta_c', h_c, pi and K form factors) have been made, and numerous high…

High Energy Physics - Experiment · Physics 2009-11-11 Kamal K. Seth

We determine the di-electron widths of the Upsilon(1S), Upsilon(2S), and Upsilon(3S) resonances with better than 2% precision by integrating the cross-section of e+e- -> Upsilon over the e+e- center-of-mass energy. Using e+e- energy scans…

High Energy Physics - Experiment · Physics 2010-04-08 CLEO Collaboration , J. L. Rosner

We report on a study of exclusive radiative decays of the Upsilon(1S) resonance into the final states gamma pi^0 pi^0, gamma eta eta and gamma pi^0 eta, using 1.13 inverse femto-barn of e^+ e^- annihilation data collected at sqrt(s)= 9.46…

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

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