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A measurement of the production of vector bottomonium states, $\varUpsilon(\textrm{1S})$, $\varUpsilon(\textrm{2S})$, and $\varUpsilon(\textrm{3S})$, in Pb+Pb and $pp$ collisions at a center-of-mass energy per nucleon pair of 5.02 TeV is…

Nuclear Experiment · Physics 2023-08-23 ATLAS Collaboration

We report a measurement of the exclusive $B^+$ meson decay to the $D_s^{(*)-} K^+\pi^+$ final state using $657 \times 10^{6} B\overline{B}$ pairs collected at the $\Upsilon(4S)$ resonance with the Belle detector at the KEKB…

High Energy Physics - Experiment · Physics 2009-10-06 The Belle Collaboration , J. Wiechczynski , T. Lesiak

We report the first observation of e+e- -> Upsilon(1S)pi+pi-, Upsilon(2S)pi+pi-, and first evidence for e+e- -> Upsilon(3S)pi+pi-, Upsilon(1S)K+K-, near the peak of the Upsilon(5S) resonance at sqrt{s}~10.87 GeV. The results are based on a…

High Energy Physics - Experiment · Physics 2009-10-26 The Belle Collaboration , K. -F. Chen , W. -S. Hou , M. Shapkin , A. Sokolov et al

The $\Upsilon(10753)$ state has been recently observed by the Belle and Belle~II collaborations with enough global significance to motivate an assessment of the high-energy spectrum usually predicted by any reasonable \emph{na\"ive} quark…

High Energy Physics - Phenomenology · Physics 2024-03-07 P. G. Ortega , D. R. Entem , F. Fernández , J. Segovia

In this paper, we model $\Upsilon(10753)$ as a $4S$-$3D$ bottomonium mixture and $\Upsilon(10860)$ as a $5S$-$4D$ mixture, and predict the properties of a new bottomonium state, $\Upsilon(10950)$, as the mixing partner of $\Upsilon(10860)$.…

High Energy Physics - Phenomenology · Physics 2025-10-20 Zheng-Li Luo , Yi-Lin Song , Feng-Kun Guo

We report the study of e+e- -> Upsilon(1S)pi+pi-, Upsilon(2S)pi+pi-, Upsilon(3S)pi+pi-, and Upsilon(1S)K+K-, near the peak of the Upsilon(5S) resonance. The results are based on a data sample of 21.7 fb^-1 collected with the Belle detector…

High Energy Physics - Experiment · Physics 2019-08-13 K. -F. Chen

Cabibbo-suppressed decays $B \to D^{(*)} K^-$ using a 10.4 fb$^{-1}$ data sample accumulated at the $\Upsilon(4S)$ resonance with the Belle detector at the KEKB $e^+ e^-$ storage ring. The high-momentum particle identification system of…

High Energy Physics - Experiment · Physics 2010-05-28 K. Abe

We study the rare hadronic transitions $\Upsilon(2S)\rightarrow \Upsilon(1S)\eta$ and $\Upsilon(2S)\rightarrow \Upsilon(1S)\pi^0$ using a sample of 158 $\times 10^6$ $\Upsilon(2S)$ decays collected with the Belle detector at the KEKB…

High Energy Physics - Experiment · Physics 2013-05-30 Belle Collaboration , U. Tamponi , R. Mussa , I. Adachi , H. Aihara , D. M. Asner , V. Aulchenko , T. Aushev , A. M. Bakich , M. Barrett , B. Bhuyan , A. Bondar , A. Bozek , M. Bra\v , T. E. Browder , A. Chen , P. Chen , B. G. Cheon , K. Chilikin , I. -S. Cho , K. Cho , Y. Choi , J. Dalseno , Z. Dole\v , Z. Drásal , D. Dutta , S. Eidelman , D. Epifanov , S. Esen , H. Farhat , J. E. Fast , A. Frey , V. Gaur , R. Gillard , Y. M. Goh , B. Golob , K. Hayasaka , Y. Horii , Y. Hoshi , H. J. Hyun , T. Iijima , A. Ishikawa , Y. Iwasaki , I. Jaegle , J. H. Kang , T. Kawasaki , H. O. Kim , J. H. Kim , K. T. Kim , M. J. Kim , Y. J. Kim , J. Klucar , B. R. Ko , P. Kody\v , S. Korpar , R. T. Kouzes , P. Kri\v , P. Krokovny , T. Kumita , A. Kuzmin , S. -H. Lee , Y. Li , C. Liu , Y. Liu , Z. Q. Liu , D. Liventsev , H. Miyata , R. Mizuk , G. B. Mohanty , A. Moll , N. Muramatsu , M. Nakao , Z. Natkaniec , C. Ng , S. Nishida , O. Nitoh , S. Ogawa , T. Ohshima , S. Okuno , S. L. Olsen , Y. Onuki , P. Pakhlov , H. K. Park , K. S. Park , T. K. Pedlar , R. Pestotnik , M. Petri\v , L. E. Piilonen , M. Röhrken , Y. Sakai , S. Sandilya , D. Santel , L. Santelj , T. Sanuki , O. Schneider , G. Schnell , C. Schwanda , K. Senyo , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , F. Simon , P. Smerkol , Y. -S. Sohn , A. Sokolov , E. Solovieva , M. Stari\v , T. Sumiyoshi , K. Tanida , N. Taniguchi , G. Tatishvili , Y. Teramoto , K. Trabelsi , S. Uehara , S. Uno , C. Van Hulse , P. Vanhoefer , G. Varner , C. H. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , K. M. Williams , E. Won , B. D. Yabsley , Y. Yamashita , C. Z. Yuan , Z. P. Zhang , V. Zhilich , V. Zhulanov , A. Zupanc

We present here a model to describe the bottomonium suppression in Pb$+$Pb collisions at Large Hadron Collider (LHC), at $\sqrt{s_{NN}}=2.76$ TeV by using the quasi-particle model (QPM) equation of state (EOS) for the Quark-Gluon Plasma…

High Energy Physics - Phenomenology · Physics 2015-02-23 S. Ganesh , Madhukar Mishra

The bottomonium spectrum is far from being established. The structures of higher vector states, including the $\Upsilon(10580)$, $\Upsilon(10860)$, and $\Upsilon(11020)$ states, are still in dispute. In addition, whether the…

High Energy Physics - Phenomenology · Physics 2020-01-30 Bing Chen , Ailin Zhang , Jin He

We report the results of a search for the bottomonium ground state eta_b(1S) in the photon energy spectrum with a sample of (109 +/- 1) million of Upsilon(3S) recorded at the Upsilon(3S) energy with the BABAR detector at the PEP-II B…

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

The cross section for e+e- to pi+ pi- psi(2S) between threshold and \sqrt{s}=5.5 GeV is measured using 673 fb^{-1} of data on and off the \Upsilon(4S) resonance collected with the Belle detector at KEKB. Two resonant structures are observed…

High Energy Physics - Experiment · Physics 2008-11-26 X. L. Wang , Belle Collaboration

We report the first observation of the decays $B^0 \rightarrow p\bar{\Lambda} D^{(*)-}$. The data sample of $711$ fb$^{-1}$ used in this analysis corresponds to $772$ million $B\bar{B}$ pairs, collected at the $\Upsilon(4S)$ resonance by…

High Energy Physics - Experiment · Physics 2015-12-02 Y. -Y. Chang , M. -Z. Wang , A. Abdesselam , I. Adachi , K. Adamczyk , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , T. Aushev , V. Babu , I. Badhrees , A. M. Bakich , E. Barberio , B. Bhuyan , J. Biswal , A. Bobrov , A. Bozek , M. Bračko , T. E. Browder , D. Červenkov , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , R. Chistov , V. Chobanova , S. -K. Choi , Y. Choi , D. Cinabro , J. Dalseno , M. Danilov , J. Dingfelder , Z. Doležal , Z. Drásal , D. Dutta , S. Eidelman , H. Farhat , J. E. Fast , T. Ferber , B. G. Fulsom , V. Gaur , N. Gabyshev , S. Ganguly , A. Garmash , R. Gillard , R. Glattauer , Y. M. Goh , P. Goldenzweig , D. Greenwald , O. Grzymkowska , J. Haba , K. Hayasaka , H. Hayashii , X. H. He , W. -S. Hou , C. -L. Hsu , T. Iijima , K. Inami , A. Ishikawa , R. Itoh , Y. Iwasaki , W. W. Jacobs , I. Jaegle , D. Joffe , K. K. Joo , T. Kawasaki , D. Y. Kim , H. J. Kim , J. B. Kim , J. H. Kim , K. T. Kim , M. J. Kim , S. H. Kim , Y. J. Kim , K. Kinoshita , S. Korpar , P. Križan , P. Krokovny , T. Kuhr , T. Kumita , A. Kuzmin , Y. -J. Kwon , Y. -T. Lai , I. S. Lee , L. Li , Y. Li , J. Libby , D. Liventsev , P. Luki , M. Masuda , K. Miyabayashi , H. Miyake , H. Miyata , R. Mizuk , G. B. Mohanty , S. Mohanty , A. Moll , H. K. Moon , T. Mori , E. Nakano , M. Nakao , T. Nanut , M. Nayak , S. Nishida , S. Ogawa , H. Ozaki , P. Pakhlov , G. Pakhlova , B. Pal , C. W. Park , T . K. Pedlar , R. Pestotnik , M. Petrič , L. E. Piilonen , J. Rauch , E. Ribežl , M. Ritter , A. Rostomyan , S. Ryu , H. Sahoo , Y. Sakai , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , I. S. Seong , M. E. Sevior , V. Shebalin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , F. Simon , Y. -S. Sohn , M. Starič , J. Stypula , M. Sumihama , K. Sumisawa , T. Sumiyoshi , U. Tamponi , K. Tanida , Y. Teramoto , T. Uglov , Y. Unno , S. Uno , Y. Usov , C. Van Hulse , P. Vanhoefer , G. Varner , V. Vorobyev , A. Vossen , M. N. Wagner , C. H. Wang , P. Wang , M. Watanabe , Y. Watanabe , K. M. Williams , E. Won , J. Yamaoka , S. Yashchenko , J. Yelton , Y. Yusa , Z. P. Zhang , V. Zhulanov , A. Zupanc

Stimulated by the exciting progress in the observation of new bottomonium states, we study the bottomonium spectrum. To calculate the mass spectrum, we adopt a nonrelativistic screened potential model. The radial Schr\"{o}dinger equation is…

High Energy Physics - Phenomenology · Physics 2017-04-12 Wei-Jun Deng , Hui Liu , Long-Cheng Gui , Xian-Hui Zhong

We study the energy spectrum of bottomonium in perturbative QCD, taking alpha_s(Mz)=0.1181 +/- 0.0020 as input and fixing m_b^{MSbar}(m_b^{MSbar}) on the Upsilon(1S) mass. Contrary to wide beliefs, perturbative QCD reproduces reasonably…

High Energy Physics - Phenomenology · Physics 2009-06-12 N. Brambilla , Y. Sumino , A. Vairo

We investigate the properties of S-and P-wave bottomonium states in the vicinity of the deconfinement transition temperature. The light degrees of freedom are represented by dynamical lattice QCD configurations of the HotQCD collaboration…

High Energy Physics - Lattice · Physics 2015-07-28 Seyong Kim , Peter Petreczky , Alexander Rothkopf

We study B- meson decays to pbar Lambda D(*)0 final states using a sample of 657 * 10^6 B Bbar events collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ e- collider. The observed branching…

High Energy Physics - Experiment · Physics 2015-05-30 P. Chen , M. -Z. Wang , I. Adachi , H. Aihara , D. M. Asner , V. Aulchenko , T. Aushev , A. M. Bakich , E. Barberio , K. Belous , B. Bhuyan , A. Bozek , M. Bračko , T. E. Browder , M. -C. Chang , P. Chang , Y. Chao , A. Chen , B. G. Cheon , I. -S. Cho , K. Cho , Y. Choi , J. Dalseno , M. Danilov , Z. Doležal , Z. Drásal , S. Eidelman , J. E. Fast , M. Feindt , V. Gaur , Y. M. Goh , J. Haba , T. Hara , K. Hayasaka , H. Hayashii , Y. Hoshi , W. -S. Hou , Y. B. Hsiung , H. J. Hyun , A. Ishikawa , R. Itoh , M. Iwabuchi , Y. Iwasaki , T. Iwashita , T. Julius , J. H. Kang , P. Kapusta , N. Katayama , T. Kawasaki , H. Kichimi , C. Kiesling , H. O. Kim , J. B. Kim , J. H. Kim , K. T. Kim , M. J. Kim , Y. J. Kim , K. Kinoshita , B. R. Ko , N. Kobayashi , S. Koblitz , P. Križan , T. Kuhr , A. Kuzmin , Y. -J. Kwon , J. S. Lange , S. -H. Lee , J. Li , Y. Li , J. Libby , C. Liu , Y. Liu , D. Liventsev , R. Louvot , D. Matvienko , S. McOnie , H. Miyata , Y. Miyazaki , G. B. Mohanty , Y. Nagasaka , E. Nakano , M. Nakao , Z. Natkaniec , S. Neubauer , S. Nishida , O. Nitoh , S. Ogawa , T. Ohshima , S. L. Olsen , Y. Onuki , P. Pakhlov , G. Pakhlova , H. Park , H. K. Park , T. K. Pedlar , R. Pestotnik , M. Peters , M. Petrič , L. E. Piilonen , M. Ritter , M. Röhrken , S. Ryu , H. Sahoo , Y. Sakai , T. Sanuki , O. Schneider , C. Schwanda , K. Senyo , M. E. Sevior , M. Shapkin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , F. Simon , J. B. Singh , P. Smerkol , Y. -S. Sohn , E. Solovieva , S. Stanič , M. Starič , M. Sumihama , T. Sumiyoshi , G. Tatishvili , Y. Teramoto , M. Uchida , S. Uehara , Y. Unno , S. Uno , G. Varner , K. E. Varvell , C. H. Wang , X. L. Wang , Y. Watanabe , K. M. Williams , E. Won , B. D. Yabsley , Y. Yamashita , M. Yamauchi , Z. P. Zhang

At least one state in the first family of D-wave $b \bar b$ quarkonium levels has been discovered near the predicted mass of 10.16 GeV/$c^2$. This state is probably the one with J=2. This state and the ones with J=1 and J=3 may contribute a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jonathan L. Rosner

We report a measurement of the exclusive $B^+$ meson decay to the final state $D_s^- K^+\pi^+$ using $520 \times 10^{6} B\bar{B}$ pairs collected near the $\Upsilon(4S)$ resonance, with the Belle detector at the KEKB asymmetric-energy…

High Energy Physics - Experiment · Physics 2007-08-22 The Belle Collaboration , K. Abe

Ground state and radial excitation mass spectra of bottomonium states are computed using the Instanton Induced $q \bar{q}$ Potential obtained from Instanton Liquid Model for QCD vacuum. The Schrodinger equation is solved for two body…

High Energy Physics - Phenomenology · Physics 2019-10-15 Bhoomika Pandya , Manan Shah , P C Vinodkumar