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Related papers: Photon transitions in Upsilon(2S) and Upsilon(3S)

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We present new measurements of photon energies and branching fractions for the radiative transitions: Upsilon(2S)->gamma+chi_b(J=0,1,2). The masses of the chi_b states are determined from the measured radiative photon energies. The ratio of…

High Energy Physics - Experiment · Physics 2010-04-08 K. Edwards

Using data collected with the CLEO-III detector at the CESR e+e- collider, we report on a first observation of the decay of the Upsilon(3S) to tau tau, and precisely measure the ratio of branching fractions of Upsilon(nS),n=1,2,3 to tau tau…

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

The Belle and Belle II experiments have collected a $1.6\,\mathrm{ab}^{-1}$ sample of $e^+e^-$ collision data at center-of-mass energies near the $\Upsilon(nS)$ resonances. We conduct searches for transitions from the spin-singlet…

High Energy Physics - Experiment · Physics 2026-03-13 S. Wallner

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

Using photon conversions to e^+e^- pairs, the energy spectrum of inclusive photons from psi(2S) radiative decays is measured by BESII at the Beijing Electron-Positron Collider. The chi_{cJ}(1P) states (J=0,1,2) are clearly observed with…

High Energy Physics - Experiment · Physics 2008-11-26 M. Ablikim , J. Z. Bai

We report the first observation of the radiative transition h_b(1P)->eta_b(1S)gamma, where the h_b(1P) is produced in Upsilon(5S)->h_b(1P)pi+pi- dipion transitions. We measure the eta_b(1S) mass to be (9401.0+-1.9+1.4-2.4)MeV/c^2 with a…

High Energy Physics - Experiment · Physics 2012-08-27 BELLE Collaboration

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

We point out some properties of the amplitude of the dipion transition $\Upsilon(3S) \to \Upsilon(1S) \pi \pi$ in relation to the recently reported results of a CLEO analysis of form factors in this amplitude. We find that the reported…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Dubynskiy , M. B. Voloshin

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

We report preliminary measurements of the first (mean) and second moment (variance) of the inclusive photon energy spectrum in $B\to X_s\gamma$ decays, for threshold values of the photon energy in the range 1.8--2.3 GeV as measured in the…

High Energy Physics - Experiment · Physics 2012-08-27 Belle 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

We review recent charmonium and bottomonium spectroscopy results from the B-factories Belle and \babar. A particular focus is given to the new $\eta_{c}(1S)$ and $\eta_{c}(2S)$ measurement and to the radiative transitions from $\Upsilon…

High Energy Physics - Experiment · Physics 2011-07-07 Valentina Santoro

We study inclusive di-pion decays using a sample of 108 x 10^6 Upsilon(3S) events recorded with the BABAR detector. We search for the decay mode Upsilon(3S) --> pi+ pi- h_b(1P) and find no evidence for the bottomonium spin-singlet state…

High Energy Physics - Experiment · Physics 2012-08-27 The BABAR Collaboration

The exclusive photoproduction of $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S) mesons is studied in their leptonic ($\mu^{+}\mu^{-}$) decay modes, in ultraperipheral pPb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. The data was recorded by…

High Energy Physics - Experiment · Physics 2019-03-27 Kousik Naskar

Using data taken with the CLEO II detector at the Cornell Electron Storage Ring, we have determined the ratio of branching fractions: $R_{\gamma} \equiv \Gamma(\Upsilon(1S) \rightarrow \gamma gg)/\Gamma(\Upsilon(1S) \rightarrow ggg) = (2.75…

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

We study transitions between Upsilon states with the emission of charged pions using 604.6/fb of data collected with the Belle detector at the KEKB asymmetric-energy e+e- collider. The measured product branching fraction is B(Upsilon(4S) ->…

High Energy Physics - Experiment · Physics 2009-10-06 The Belle Collaboration , A. Sokolov , M. Shapkin

Using e+e- collision data taken with the CLEO-c detector at the Cornell Electron Storage Ring, we have investigated the direct photon spectrum in the decay psi(2S)->gamma+gluon+gluon. We determine the ratio R of that inclusive direct photon…

High Energy Physics - Experiment · Physics 2019-08-13 J. Libby

We report evidence for the ground state of bottomonium, eta_b(1S), in the radiative decay Upsilon(3S) --> gamma eta_b in e^+e^- annihilation data taken with the CLEO III detector. Using 6 million Upsilon(3S) decays, and assuming…

In order to explain the observed unusually large dipion transition rates of $\Upsilon(10870)$, the scalar resonance contributions in the re-scattering model to the dipion transitions of $\Upsilon(4S)$ and $\Upsilon(5S)$ are studied. Since…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ce Meng , Kuang-Ta Chao

We present the first evidence for the production of Upsilon(1D) states in the four-photon cascade, Upsilon(3S)-->gamma chib(2P), chib(2P)-->gamma Upsilon(1D), Upsilon(1D)-->gamma chib(1P), chib(1P)-->gamma Upsilon(1S), followed by the…

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