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We estimate the most important corrections to the branching ratios for the invisible decays of quarkonium states, arising from possible extensions of the standard model. Among the possibilities considered are the presence of extra Z-bosons,…

High Energy Physics - Phenomenology · Physics 2009-10-31 Lay Nam Chang , Oleg Lebedev , John N. Ng

Following searches for photinos and very light gravitinos in invisible decays of psi and Upsilon, we discuss new limits on Light Dark Matter and U bosons, from psi and Upsilon decays, as well as rare decays of K+ and invisible decays of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Pierre Fayet

Hidden sectors with light extra U(1) gauge bosons, so-called hidden photons, have recently attracted some attention because they are a common feature of physics beyond the Standard Model like string theory and supersymmetry and additionally…

High Energy Physics - Phenomenology · Physics 2012-11-20 Sarah Andreas , Carsten Niebuhr , Andreas Ringwald

Radiative magnetic dipole decays of heavy-light vector mesons into pseudoscalar mesons V -> P\gamma are considered within the relativistic quark model. The light quark is treated completely relativistically, while for the heavy quark the…

High Energy Physics - Phenomenology · Physics 2009-11-07 D. Ebert , R. N. Faustov , V. O. Galkin

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

In this lecture we show that the study of hadronic resonances is severely hampered by the lack of accurate data and, moreover, that for similar reason the study of Weak substructure does not make sufficient progress. We furthermore report…

High Energy Physics - Phenomenology · Physics 2017-12-19 Eef van Beveren , Susana Coito , George Rupp

We present a measurement of the branching fraction of invisible Upsilon(1S) decays, using 1.2 fb^{-1} of data collected at the Upsilon(2S) resonance with the CLEO III detector at CESR. After subtracting expected backgrounds from events that…

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

Light scalars appear in many well-motivated extensions of the Standard Model including supersymmetric models with additional gauge singlets. Such scalars could mediate the interactions between dark matter and nuclei, giving rise to the…

High Energy Physics - Phenomenology · Physics 2013-12-18 Kai Schmidt-Hoberg , Florian Staub , Martin Wolfgang Winkler

A non-standard light CP-odd Higgs boson could induce a slight (but observable) lepton universality breakdown in Upsilon leptonic decays. Moreover, the mixing between such a pseudoscalar Higgs and $\eta_b$ states might shift the mass levels…

High Energy Physics - Phenomenology · Physics 2009-11-10 Miguel A. Sanchis-Lozano

Recently CLEO has studied the radiative decay of $\Upsilon$ into $\eta'$ and an upper limit for the decay has been determined. Confronting with this upper limit,most of theoretical predictions for the decay fails. After briefly reviewing…

High Energy Physics - Phenomenology · Physics 2009-11-07 J. P. Ma

A non-standard CP-odd Higgs boson could induce a slight (but observable) lepton universality breaking in Upsilon leptonic decays. Moreover, mixing between such a pseudoscalar Higgs boson and $\eta_b$ states might shift their mass levels,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Miguel-Angel Sanchis-Lozano

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

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

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

The $SU(3)$-violating decays $\Phi^{2S} \goto \Phi^{1S} X$, where $X = \pi^0$ or $\eta$ and $\Phi = J/\psi$ or $\Upsilon$ have been recently proposed as a means of probing the light quark masses beyond leading order in chiral perturbation…

High Energy Physics - Phenomenology · Physics 2009-09-15 Markus A. Luty , Raman Sundrum

We search for evidence of a light Higgs boson (A0) in the radiative decays of the narrow Upsilon(3S) resonance: Upsilon(3S) -> gamma A0, where A0 -> invisible or A0 -> mu+mu-. Such an object appears in extensions of the Standard Model,…

High Energy Physics - Experiment · Physics 2014-11-20 Swagato Banerjee

The Higgs boson recently discovered at the Large Hadron Collider has shown to have couplings to the remaining particles well within what is predicted by the Standard Model. The search for other new heavy scalar states has so far revealed to…

High Energy Physics - Phenomenology · Physics 2015-06-17 A. Arhrib , P. M. Ferreira , R. Santos

Using 3.1 fb$^{-1}$ of data accumulated at the $\Upsilon$(4S) by the CLEO-II detector, corresponding to 3.3 million $B\bar{B}$ pairs, we have searched for the color-suppressed $B$ hadronic decay processes: $\bar{B}^0 \to D^0 (D^{*0}) X^0$,…

High Energy Physics - Experiment · Physics 2010-04-08 CLEO Collaboration , B. Nemati et al

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

Among the many unresolved questions in light quark spectroscopy, the underlying structure of the scalar mesons and the identification of states with a gluonic content rank high. Recently, new information has come from $\phi$ radiative…

High Energy Physics - Experiment · Physics 2011-02-01 Brian T. Meadows