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Related papers: Upsilon Decays

200 papers

The experimental status of stable bound states made out of heavy quarks is reviewed. The need for a way to deal with the non-perturbative transitions involved calls for precision measurements on one hand, and for discovery of as yet…

High Energy Physics - Experiment · Physics 2014-11-17 Hanna Mahlke

The three lowest-lying $\Upsilon$ states, i.e. $\Upsilon(1S)$, $\Upsilon(2S)$, and $\Upsilon(3S)$, composed of $b\bar b$ pairs and below the $B\bar B$ threshold, provide a good platform for the researches of hadronic physics and physics…

High Energy Physics - Experiment · Physics 2020-08-11 Sen Jia , Xingyu Zhou , Chengping Shen

Using data collected using the CLEO III detector, we present recent results on decays of the $\Upsilon(1S)-\Upsilon(3S)$ resonances. We report on three analyses. They are: (1) improved measurements of the muonic branching fraction of the…

High Energy Physics - Experiment · Physics 2019-08-14 Steven R. Blusk

Recent CLEO results on the observation of the $\Upsilon(1D)$ state and a search for the $\eta_b(1S)$ state from a data sample of $4.7 \times 10^6\,\Upsilon(3S)$ decays collected with the CLEO-III detector, and a measurement of the…

High Energy Physics - Experiment · Physics 2007-05-23 Thomas E. Coan

Recent results on the QCD analysis of bound states of heavy $\bar{q}q$ quarks are reviewed, paying attention to what can be derived from the theory with a reasonable degree of rigour. We report a calculation of $\bar{b}c$ bound states; a…

High Energy Physics - Phenomenology · Physics 2011-01-27 F. J. Yndurain

We examine the electronic width ratios of Upsilon resonances below the BBbar threshold by means of an effective (Cornell-type) QCD potential incorporating 1/m_b corrections obtained from a prior fit to the bottomonium spectrum. From our…

High Energy Physics - Phenomenology · Physics 2008-11-26 Juan-Luis Domenech-Garret , Miguel-Angel Sanchis-Lozano

Bound states of heavy $\bar{q}q$ quarks are reviewed within the context of QCD. First of all, we consider the calculations which can be performed {\sl ab initio}, which includes $\bar{t}t$ with principal quantum number $n$ up to four,…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. J. Yndurain

Using data taken with the CLEO III detector, 1.09 fb-1 at Upsilon(1S), and 1.28 fb-1 at Upsilon(2S), branching fractions have been measured for the first time for exclusive decays of each resonance into one hundred different final states…

High Energy Physics - Experiment · Physics 2015-06-05 S. Dobbs , Z. Metreveli , A. Tomaradze , T. Xiao , Kamal K. Seth

The potential of decays of mesons containing heavy quarks [including $B$ mesons and the $\Upsilon(1S)$] for producing final states of matter with unusual quark configurations, such as $q q \bar q \bar q$ or $q q q q \bar q$, is…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jonathan L. Rosner

Recent investigations have suggested that the six-quark combination uuddss could be a deeply bound state (S) that has eluded detection so far, and a potential dark matter candidate. We report the first search for a stable, doubly strange…

High Energy Physics - Experiment · Physics 2019-03-06 Bertrand Echenard

We review selected recent Belle results in quarkonium physics, that include precision measurement of the eta_b(1S) parameters, evidence for the eta_b(2S); evidence for the psi_2(1D); observation of the psi(4040) and psi(4160) transitions to…

High Energy Physics - Experiment · Physics 2013-03-26 Roman Mizuk

Based on the non-relativistic QCD factorization scheme, we study the hadroproduction of the bottomonium states $\Upsilon(5S)$ and $\Upsilon(6S)$. We argue to search for them in the final states $\Upsilon(1S,2S,3S)\pi^+\pi^-$, which are…

High Energy Physics - Phenomenology · Physics 2013-10-02 Ahmed Ali , Christian Hambrock , Wei Wang

We present final measurements of thirteen charmless hadronic B decay modes from the CLEO experiment. The decay modes include the ten pipi, Kpi, and KKbar final states and new limits on dibaryonic final states, ppbar, pLambdabar, and…

High Energy Physics - Experiment · Physics 2019-08-18 A. Bornheim

I detail recent work done by the CLEO collaboration using data gathered at the CESR accelerator concerning the Upsilon system. Results include B_S production at the Upsilon(5S), decays of the Upsilon(nS) (n=1,2,3) to tau pairs, the Upsilon…

High Energy Physics - Experiment · Physics 2019-08-14 Jean Duboscq

The bottomonium and charmonium systems have long proved to be a rich source of QCD physics. Recent CLEO contributions in three disparate areas are presented: (1) the study of quark and gluon hadronization using $\Upsilon$ decays; (2) the…

High Energy Physics - Experiment · Physics 2007-05-23 R. E. Mitchell

Using data obtained with the CLEO~III detector, running at the Cornell Electron Storage Ring (CESR), we report on a new study of exclusive radiative Upsilon(1S) decays into the final states gamma pi^+ pi^-, gamma K^+ K^-, and gamma p pbar..…

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

We search for bottomonium states in Upsilon(2S)-> (bb-bar) gamma decays with an integrated luminosity of 24.7fb^-1 recorded at the Upsilon(2S) resonance with the Belle detector at KEK, containing (157.8+-3.6) X 10^6 Upsilon(2S) events. The…

High Energy Physics - Experiment · Physics 2013-09-11 Belle Collaboration , S. Sandilya , K. Trabelsi , G. B. Mohanty , I. Adachi , H. Aihara , D. M. Asner , T. Aushev , A. M. Bakich , A. Bala , V. Bhardwaj , B. Bhuyan , A. Bondar , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , P. Chen , B. G. Cheon , K. Chilikin , R. Chistov , K. Cho , V. Chobanova , S. -K. Choi , Y. Choi , D. Cinabro , J. Dalseno , J. Dingfelder , Z. Doležal , A. Drutskoy , D. Dutta , S. Eidelman , H. Farhat , J. E. Fast , M. Feindt , T. Ferber , A. Frey , V. Gaur , N. Gabyshev , S. Ganguly , R. Gillard , Y. M. Goh , B. Golob , J. Haba , T. Hara , K. Hayasaka , H. Hayashii , Y. Hoshi , W. -S. Hou , Y. B. Hsiung , H. J. Hyun , T. Iijima , A. Ishikawa , R. Itoh , Y. Iwasaki , T. Julius , D. H. Kah , J. H. Kang , E. Kato , H. Kawai , T. Kawasaki , C. Kiesling , D. Y. Kim , H. O. Kim , J. B. Kim , J. H. Kim , Y. J. Kim , J. Klucar , B. R. Ko , P. Kodyš , S. Korpar , P. Križan , P. Krokovny , T. Kumita , A. Kuzmin , Y. -J. Kwon , J. S. Lange , S. -H. Lee , J. Li , Y. Li , Z. Q. Liu , D. Liventsev , P. Lukin , J. MacNaughton , D. Matvienko , K. Miyabayashi , H. Miyata , R. Mizuk , A. Moll , N. Muramatsu , R. Mussa , Y. Nagasaka , M. Nakao , M. Nayak , C. Ng , N. K. Nisar , S. Nishida , O. Nitoh , S. Ogawa , S. Okuno , C. Oswald , G. Pakhlova , C. W. Park , H. Park , H. K. Park , T. K. Pedlar , R. Pestotnik , M. Petrič , L. E. Piilonen , M. Ritter , M. Röhrken , A. Rostomyan , S. Ryu , H. Sahoo , T. Saito , K. Sakai , Y. Sakai , L. Santelj , T. Sanuki , Y. Sato , V. Savinov , O. Schneider , G. Schnell , D. Semmler , K. Senyo , M. E. Sevior , M. Shapkin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , Y. -S. Sohn , A. Sokolov , E. Solovieva , S. Stanič , M. Starič , M. Steder , T. Sumiyoshi , U. Tamponi , K. Tanida , G. Tatishvili , Y. Teramoto , T. Tsuboyama , M. Uchida , S. Uehara , T. Uglov , Y. Unno , S. Uno , P. Urquijo , S. E. Vahsen , C. Van Hulse , P. Vanhoefer , G. Varner , V. Vorobyev , M. N. Wagner , C. H. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , J. Wiechczynski , K. M. Williams , E. Won , B. D. Yabsley , J. Yamaoka , Y. Yamashita , S. Yashchenko , C. Z. Yuan , Y. Yusa , C. C. Zhang , Z. P. Zhang , V. Zhilich , A. Zupanc

We search for $\Xi^0p$, $\Omega^-p$, and $\Omega^-n$ dibaryon states in $\Upsilon(1S)$ and $\Upsilon(2S)$ decays, probing mass regions near the corresponding baryon-pair thresholds. Multistrange baryon-baryon interactions are relevant to…

High Energy Physics - Experiment · Physics 2026-05-29 Belle , Belle II Collaborations , : , M. Abumusabh , I. Adachi , A. Aggarwal , Y. Ahn , H. Aihara , N. Akopov , S. Alghamdi , M. Alhakami , N. Althubiti , K. Amos , N. Anh Ky , H. Atmacan , V. Aushev , R. Ayad , V. Babu , H. Bae , N. K. Baghel , P. Bambade , Sw. Banerjee , M. Bartl , J. Baudot , A. Beaubien , F. Becherer , J. Becker , G. F. Benfratello , J. V. Bennett , V. Bertacchi , M. Bertemes , E. Bertholet , M. Bessner , S. Bettarini , V. Bhardwaj , F. Bianchi , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , G. Bonvicini , J. Borah , A. Boschetti , M. Bračko , P. Branchini , R. A. Briere , T. E. Browder , A. Budano , S. Bussino , F. Callet , Q. Campagna , M. Campajola , L. Cao , G. Casarosa , C. Cecchi , M. -C. Chang , P. Cheema , L. Chen , B. G. Cheon , C. Cheshta , H. Chetri , K. Chilikin , K. Chirapatpimol , H. -E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , S. Choudhury , S. Chutia , J. Cochran , J. A. Colorado-Caicedo , I. Consigny , L. Corona , H. Crotte Ledesma , S. Cuccuini , J. X. Cui , E. De La Cruz-Burelo , S. A. De La Motte , G. De Nardo , G. De Pietro , R. de Sangro , M. Destefanis , S. Dey , R. Dhayal , A. Di Canto , J. Dingfelder , Z. Doležal , X. Dong , M. Dorigo , K. Dugic , G. Dujany , P. Ecker , J. Eppelt , R. Farkas , P. Feichtinger , T. Ferber , T. Fillinger , C. Finck , F. Forti , A. Frey , B. G. Fulsom , A. Gabrielli , E. Ganiev , R. Garg , G. Gaudino , V. Gaur , V. Gautam , A. Gellrich , G. Ghevondyan , D. Ghosh , H. Ghumaryan , R. Giordano , A. Giri , P. Gironella Gironell , B. Gobbo , R. Godang , O. Gogota , W. Gradl , E. Graziani , D. Greenwald , Y. Guan , K. Gudkova , I. Haide , Y. Han , K. Hayasaka , H. Hayashii , S. Hazra , M. T. Hedges , A. Heidelbach , G. Heine , I. Heredia de la Cruz , T. Higuchi , M. Hoek , M. Hohmann , R. Hoppe , P. Horak , X. T. Hou , C. -L. Hsu , T. Humair , T. Iijima , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , P. Jackson , D. Jacobi , W. W. Jacobs , E. -J. Jang , S. Jia , Y. Jin , A. Johnson , K. K. Joo , K. H. Kang , G. Karyan , C. Kiesling , C. Kim , D. Y. Kim , H. Kim , J. -Y. Kim , K. -H. Kim , K. Kinoshita , P. Kodyš , T. Koga , S. Kohani , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , P. Krokovny , T. Kuhr , Y. Kulii , R. Kumar , T. Kunigo , S. Kurokawa , Y. -J. Kwon , T. Lam , J. S. Lange , T. S. Lau , R. Leboucher , H. Lee , M. J. Lee , P. Leo , P. M. Lewis , C. Li , Q. M. Li , S. X. Li , W. Z. Li , Y. Li , Y. B. Li , J. Libby , J. Lin , Z. Liptak , C. Liu , M. H. Liu , Q. Y. Liu , Z. Q. Liu , S. Longo , A. Lozar , J. L. Ma , Y. Ma , M. Maggiora , S. P. Maharana , R. Maiti , G. Mancinelli , R. Manfredi , E. Manoni , M. Mantovano , D. Marcantonio , S. Marcello , M. Marfoli , C. Marinas , A. Martens , T. Martinov , L. Massaccesi , M. Masuda , T. Matsuda , D. Matvienko , M. Maushart , J. A. McKenna , Z. Mediankin Gruberová , R. Mehta , F. Meier , D. Meleshko , M. Merola , C. Miller , M. Mirra , K. Miyabayashi , H. Miyake , R. Mizuk , G. B. Mohanty , S. Moneta , H. -G. Moser , N. Mudgal , Th. Muller , H. Murakami , R. Mussa , M. Nakao , Z. Natkaniec , A. Natochii , M. Neu , M. Niiyama , S. Nishida , R. Nomaru , S. Ogawa , H. Ono , Y. Onuki , G. Pakhlova , S. Pardi , J. Park , K. Park , S. -H. Park , S. Patra , T. K. Pedlar , R. Pestotnik , M. Piccolo , L. E. Piilonen , P. L. M. Podesta-Lerma , T. Podobnik , A. Prakash , C. Praz , S. Prell , E. Prencipe , M. T. Prim , H. Purwar , P. Rados , S. Raiz , K. Ravindran , J. U. Rehman , M. Reif , S. Reiter , L. Reuter , D. Ricalde Herrmann , I. Ripp-Baudot , G. Rizzo , S. H. Robertson , J. M. Roney , A. Rostomyan , N. Rout , S. Saha , D. A. Sanders , S. Sandilya , L. Santelj , C. Santos , V. Savinov , B. Scavino , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , J. Serrano , M. E. Sevior , C. Sfienti , C. P. Shen , X. D. Shi , T. Shillington , T. Shimasaki , J. -G. Shiu , D. Shtol , B. Shwartz , A. Sibidanov , F. Simon , J. Skorupa , A. Soffer , A. Sokolov , E. Solovieva , S. Spataro , K. Špenko , B. Spruck , M. Starič , P. Stavroulakis , S. Stefkova , R. Stroili , M. Sumihama , M. Takahashi , M. Takizawa , U. Tamponi , K. Tanida , F. Testa , A. Thaller , D. V. Thanh , T. Tien Manh , O. Tittel , R. Tiwary , E. Torassa , F. F. Trantou , I. Tsaklidis , M. Uchida , I. Ueda , K. Unger , Y. Unno , K. Uno , S. Uno , Y. Ushiroda , S. E. Vahsen , R. van Tonder , K. E. Varvell , M. Veronesi , V. S. Vismaya , L. Vitale , V. Vobbilisetti , R. Volpe , M. Wakai , S. Wallner , M. -Z. Wang , A. Warburton , S. Watanuki , C. Wessel , X. P. Xu , B. D. Yabsley , S. Yamada , W. P. Yan , J. Yelton , K. Yi , J. H. Yin , K. Yoshihara , C. Z. Yuan , J. Yuan , L. Yuan , Y. Yusa , L. Zani , M. Zeyrek , B. Zhang , X. Zhao , V. Zhilich , J. S. Zhou , Q. D. Zhou , X. Y. Zhou , L. Zhu , R. Žlebčík

My report consists of two parts: (1). Using samples of 102 million $\Upsilon(1S)$ and 158 million $\Upsilon(2S)$ events at Belle, we study 17 exclusive hadronic decays of these two bottomonium resonances to some Vector-Pseudoscalar (VP),…

High Energy Physics - Experiment · Physics 2019-08-21 Chengping Shen

Quarkonium is the bound state of a heavy quark and its anti-quark counterpart. The study of this system has experienced a renaissance thanks to results from e+e- collider experiments, including discoveries of long-predicted conventional…

High Energy Physics - Experiment · Physics 2017-10-03 Bryan Fulsom
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