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Related papers: Bottomonium Spectroscopy at CLEO

200 papers

The recently observed by CLEO cascade decays Upsilon(3S) -> gamma chi_{bJ}^\prime -> gamma omega Upsilon are discussed. It is shown that within the nonrelativistic description of bottomonium in the heavy b quark limit, the ratio of the…

High Energy Physics - Phenomenology · Physics 2011-01-27 M. B. Voloshin

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

A universal description of the hyperfine splittings (HFS) in bottomonium and the $B_q (q=n,s,c)$ mesons is obtained with a universal strong coupling constant $\alpha_s(\mu)=0.305(2)$ in a spin-spin potential. Other characteristics are…

High Energy Physics - Phenomenology · Physics 2014-11-20 A. M. Badalian , B. L. G. Bakker , I. V. Danilkin

As tests of QCD in the bottomonium system, we give the most accurate results to date for the ground-state hyperfine splitting and the $\Upsilon$ leptonic width from full lattice QCD. These quantities are both accurately known from…

High Energy Physics - Lattice · Physics 2021-11-12 C. T. H. Davies , D. Hatton , J. Koponen , G. P. Lepage , A. T. Lytle

We present studies in bottomonium spectroscopy carried out with samples of $(98\pm1)$ million $\Upsilon(2S)$ and $(121\pm1)$ million $\Upsilon(3S)$ events recorded with the BaBar detector at the PEP-II asymmetric-energy $e^+ e^-$ collider…

High Energy Physics - Experiment · Physics 2011-10-04 V. Ziegler

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

Originally designed for CP violation studies in the B meson system, the B-Factories recently showed an exciting capability for improving our experimental knowledge in the field of hadron spectroscopy. Here I will present some of the most…

High Energy Physics - Experiment · Physics 2019-08-13 Francesco Renga

We have performed a search for the eta_b(1S) meson in the radiative decay of the Upsilon(2S) resonance using a sample of 91.6 million Upsilon(2S) events recorded with the BABAR detector at the PEP-II B factory at the SLAC National…

High Energy Physics - Experiment · Physics 2010-04-12 The BABAR Collaboration , B. Aubert

The decay branching fractions of the three narrow Upsilon resonances to mu+mu- have been measured by analyzing about 4.3 1/fb e+e- data collected in the vicinity of the resonances with the CLEO III detector. The branching fraction B(Y(1S)…

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

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

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

We use 111+/-1 million Upsilon(3S) and 89+/-1 million Upsilon(2S) events recorded by the BaBar detector at the PEP-II B-factory at SLAC to perform a study of radiative transitions between bottomonium states using photons that have been…

High Energy Physics - Experiment · Physics 2011-12-23 The BABAR Collaboration , J. P. Lees , V. Poireau , E. Prencipe , V. Tisserand , J. GarraTico , E. Grauges , M. Martinelli , D. A. Milanes , A. Palano , M. Pappagallo , G. Eigen , B. Stugu , L. Sun , D. N. Brown , L. T. Kerth , Yu. G. Kolomensky , G. Lynch , H. Koch , T. Schroeder , D. J. Asgeirsson , C. Hearty , T. S. Mattison , J. A. McKenna , A. Khan , V. E. Blinov , A. R. Buzykaev , V. P. Druzhinin , V. B. Golubev , E. A. Kravchenko , A. P. Onuchin , S. I. Serednyakov , Yu. I. Skovpen , E. P. Solodov , K. Yu. Todyshev , A. N. Yushkov , M. Bondioli , S. Curry , D. Kirkby , A. J. Lankford , M. Mandelkern , D. P. Stoker , H. Atmacan , J. W. Gary , F. Liu , O. Long , G. M. Vitug , C. Campagnari , T. M. Hong , D. Kovalskyi , J. D. Richman , C. A. West , A. M. Eisner , J. Kroseberg , W. S. Lockman , A. J. Martinez , T. Schalk , B. A. Schumm , A. Seiden , C. H. Cheng , D. A. Doll , B. Echenard , K. T. Flood , D. G. Hitlin , P. Ongmongkolkul , F. C. Porter , A. Y. Rakitin , R. Andreassen , M. S. Dubrovin , B. T. Meadows , M. D. Sokoloff , P. C. Bloom , W. T. Ford , A. Gaz , M. Nagel , U. Nauenberg , J. G. Smith , S. R. Wagner , R. Ayad , W. H. Toki , B. Spaan , M. J. Kobel , K. R. Schubert , R. Schwierz , D. Bernard , M. Verderi , P. J. Clark , S. Playfer , J. E. Watson , D. Bettoni , C. Bozzi , R. Calabrese , G. Cibinetto , E. Fioravanti , I. Garzia , E. Luppi , M. Munerato , M. Negrini , L. Piemontese , R. Baldini-Ferroli , A. Calcaterra , R. deSangro , G. Finocchiaro , M. Nicolaci , S. Pacetti , P. Patteri , I. M. Peruzzi , M. Piccolo , M. Rama , A. Zallo , R. Contri , E. Guido , M. LoVetere , M. R. Monge , S. Passaggio , C. Patrignani , E. Robutti , B. Bhuyan , V. Prasad , C. L. Lee , M. Morii , A. J. Edwards , A. Adametz , J. Marks , U. Uwer , F. U. Bernlochner , M. Ebert , H. M. Lacker , T. Lueck , P. D. Dauncey , M. Tibbetts , P. K. Behera , U. Mallik , C. Chen , J. Cochran , H. B. Crawley , W. T. Meyer , S. Prell , E. I. Rosenberg , A. E. Rubin , A. V. Gritsan , Z. J. Guo , N. Arnaud , M. Davier , D. Derkach , G. Grosdidier , F. LeDiberder , A. M. Lutz , B. Malaescu , P. Roudeau , M. H. Schune , A. Stocchi , G. Wormser , D. J. Lange , D. M. Wright , I. Bingham , C. A. Chavez , J. P. Coleman , J. R. Fry , E. Gabathuler , D. E. Hutchcroft , D. J. Payne , C. Touramanis , A. J. Bevan , F. DiLodovico , R. Sacco , M. Sigamani , G. Cowan , S. Paramesvaran , D. N. Brown , C. L. Davis , A. G. Denig , M. Fritsch , W. Gradl , A. Hafner , K. E. Alwyn , D. Bailey , R. J. Barlow , G. Jackson , G. D. Lafferty , R. Cenci , B. Hamilton , A. Jawahery , D. A. Roberts , G. Simi , C. Dallapiccola , E. Salvati , R. Cowan , D. Dujmic , G. Sciolla , D. Lindemann , P. M. Patel , S. H. Robertson , M. Schram , P. Biassoni , A. Lazzaro , V. Lombardo , F. Palombo , S. Stracka , L. Cremaldi , R. Godang , R. Kroeger , P. Sonnek , D. J. Summers , X. Nguyen , P. Taras , G. De Nardo , D. Monorchio , G. Onorato , C. Sciacca , G. Raven , H. L. Snoek , C. P. Jessop , K. J. Knoepfel , J. M. LoSecco , W. F. Wang , K. Honscheid , R. Kass , J. Brau , R. Frey , N. B. Sinev , D. Strom , E. Torrence , E. Feltresi , N. Gagliardi , M. Margoni , M. Morandin , M. Posocco , M. Rotondo , F. Simonetto , R. Stroili , E. Ben-Haim , M. Bomben , G. R. Bonneaud , H. Briand , G. Calderini , J. Chauveau , O. Hamon , Ph. Leruste , G. Marchiori , J. Ocariz , S. Sitt , M. Biasini , E. Manoni , A. Rossi , C. Angelini , G. Batignani , S. Bettarini , M. Carpinelli , G. Casarosa , A. Cervelli , F. Forti , M. A. Giorgi , A. Lusiani , N. Neri , B. Oberhof , E. Paoloni , A. Perez , G. Rizzo , J. J. Walsh , D. LopesPegna , C. Lu , J. Olsen , A. J. S. Smith , A. V. Telnov , F. Anulli , G. Cavoto , R. Faccini , F. Ferrarotto , F. Ferroni , M. Gaspero , L. LiGioi , M. A. Mazzoni , G. Piredda , C. Bunger , T. Hartmann , T. Leddig , H. Schroder , R. Waldi , T. Adye , E. O. Olaiya , F. F. Wilson , S. Emery , G. Hamel de Monchenault , G. Vasseur , Ch. Yeche , D. Aston , D. J. Bard , R. Bartoldus , J. F. Benitez , C. Cartaro , M. R. Convery , J. Dorfan , G. P. Dubois-Felsmann , W. Dunwoodie , R. C. Field , M. Franco Sevilla , B. G. Fulsom , A. M. Gabareen , M. T. Graham , P. Grenier , C. Hast , W. R. Innes , M. H. Kelsey , H. Kim , P. Kim , M. L. Kocian , D. W. G. S. Leith , P. Lewis , S. Li , B. Lindquist , S. Luitz , V. Luth , H. L. Lynch , D. B. MacFarlane , D. R. Muller , H. Neal , S. Nelson , I. Ofte , M. Perl , T. Pulliam , B. N. Ratcliff , A. Roodman , A. A. Salnikov , V. Santoro , R. H. Schindler , A. Snyder , D. Su , M. K. Sullivan , J. Va'vra , A. P. Wagner , M. Weaver , W. J. Wisniewski , M. Wittgen , D. H. Wright , H. W. Wulsin , A. K. Yarritu , C. C. Young , V. Ziegler , W. Park , M. V. Purohit , R. M. White , J. R. Wilson , A. Randle-Conde , S. J. Sekula , M. Bellis , P. R. Burchat , T. S. Miyashita , M. S. Alam , J. A. Ernst , R. Gorodeisky , N. Guttman , D. R. Peimer , A. Soffer , P. Lund , S. M. Spanier , R. Eckmann , J. L. Ritchie , A. M. Ruland , C. J. Schilling , R. F. Schwitters , B. C. Wray , J. M. Izen , X. C. Lou , F. Bianchi , D. Gamba , L. Lanceri , L. Vitale , N. Lopez-March , F. Martinez-Vidal , A. Oyanguren , H. Ahmed , J. Albert , Sw. Banerjee , H. H. F. Choi , G. J. King , R. Kowalewski , M. J. Lewczuk , C. Lindsay , I. M. Nugent , J. M. Roney , R. J. Sobie , T. J. Gershon , P. F. Harrison , T. E. Latham , E. M. T. Puccio , H. R. Band , S. Dasu , Y. Pan , R. Prepost , C. O. Vuosalo , S. L. Wu

The decay branching fractions of the three narrow Upsilon resonances to mu+ mu- have been measured by analyzing about 4.3 1/fb e+e- data collected with the CLEO III detector. The branching fraction B(Y(1S) -> mu+ mu-) = (2.49 +- 0.02 +-…

High Energy Physics - Experiment · Physics 2007-05-23 Istvan Danko

As a sister work of Ref.[1], we incorporate the color-screening effect due to light quark pair creation into the heavy quark-antiquark potential, and investigate the effects of screened potential on the spectrum of bottomonium. We calculate…

High Energy Physics - Phenomenology · Physics 2009-11-30 Bai-Qing Li , Kuang-Ta Chao

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

Hyperfine splittings (HFS) are calculated within the Field Correlator Method, taking into account relativistic corrections. The HFS in bottomonium and the $B_q$ (q=n,s) mesons are shown to be in full agreement with experiment if a universal…

High Energy Physics - Phenomenology · Physics 2011-05-05 A. M. Badalian , B. L. G. Bakker , I. V. Danilkin

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

Predictions for the hyperfine splitting of 2S bottomonia are compared with the two recent experimental candidates for the \eta_b(2S). The smaller splitting of the Belle state is consistent with unquenched lattice QCD computations, many…

High Energy Physics - Phenomenology · Physics 2013-05-30 T. J. Burns

A study of various bottomonium states, in Y(2S)-> gamma (b b-bar) decays, reconstructed exclusively in 26 hadronic final states is presented. The study is performed using a data sample recorded at the Y(2S) resonance with the Belle detector…

High Energy Physics - Experiment · Physics 2014-01-21 S. Sandilya

We search for evidence of a light scalar boson in the radiative decays of the Upsilon(2S) and Upsilon(3S) resonances: Upsilon(2S,3S)-> gamma A0, A0 -> mu^+ mu^-. Such a particle appears in extensions of the Standard Model, where a light…

High Energy Physics - Experiment · Physics 2010-04-12 The BABAR Collaboration , B. Aubert