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I review recent calculations of the suppression of bottomonium states in heavy ion collisions. A non-relativistic potential is used which is complex valued. This allows one to extract the binding energies and decay widths of the ground and…

Nuclear Theory · Physics 2013-05-14 Michael Strickland

We estimate the sum of the $\Upsilon \bar BB $ couplings using QCD Spectral Sum Rules (QSSR). Our result implies the phenomenological bound $\xi'(vv'=1) \geq -1.04$ for the slope of the Isgur-Wise function. An analytic estimate of the…

High Energy Physics - Phenomenology · Physics 2010-11-01 S. Narison

Recent data on e(-)+e(+)-->b+anti-b by the BABAR Collaboration [B. Aubert et al, Phys. Rev. Lett. 102, 012001 (2009), arXiv:0809.4120] in the energy range delimited by the B+anti-B and Lambda(b)(+)+Lambda(b)(-) thresholds are analyzed in a…

High Energy Physics - Phenomenology · Physics 2009-10-07 Eef van Beveren , George Rupp

Various sum rules for multiple giant dipole resonance states are derived. For the triple giant dipole resonance states, the energy-weighted sum of the transition strengths requires a model to be related to those of the single and double…

Nuclear Theory · Physics 2009-11-11 H. Kurasawa , T. Suzuki , P. F. Bortignon

A search for the decays of the Higgs and $Z$ bosons to $J/\psi\gamma$ and $\Upsilon(nS)\gamma$ ($n=1,2,3$) is performed with $pp$ collision data samples corresponding to integrated luminosities of up to $20.3\mathrm{fb}^{-1}$ collected at…

High Energy Physics - Experiment · Physics 2015-04-01 ATLAS Collaboration

Dynamics of hadro-quarkonium system is formulated, based on the channel coupling of a light hadron (h) and heavy quarkonium (Q\bar{Q}) to intermediate open-flavor heavy-light mesons (Q\bar{q}, \bar{Q}q). The resulting effective interaction…

High Energy Physics - Phenomenology · Physics 2014-01-21 I. V. Danilkin , V. D. Orlovsky , Yu. A. Simonov

We use the method of light-cone sum rules to study decay properties of $P$-wave bottom baryons belonging to the $SU(3)$ flavor $\mathbf{6}_F$ representation. In Ref.~\cite{Cui:2019dzj} we have studied their mass spectrum and pionic decays,…

High Energy Physics - Phenomenology · Physics 2020-03-25 Hui-Min Yang , Hua-Xing Chen , Er-Liang Cui , Atsushi Hosaka , Qiang Mao

Great strides have been made in the understanding of bound states of a bottom quark $b$ and its antiquark $\bar b$ since the discovery of the first $\Upsilon$ resonances in 1977. These {\it bottomonium} bound states have a rich spectrum…

High Energy Physics - Experiment · Physics 2017-08-23 Claudia Patrignani , Todd K. Pedlar , Jonathan L. Rosner

Inspired by the potential prospects of high-luminosity dedicated colliders and the high enthusiasms in searching for new physics in the flavor sector at the intensity frontier, the ${\Upsilon}(1S)$ ${\to}$ $D^{-}{\pi}^{+}$,…

High Energy Physics - Phenomenology · Physics 2021-02-23 Yueling Yang , Mingfei Duan , Junliang Lu , Jinshu Huang , Junfeng Sun

The CLEO Collaboration has made the first observations of hadronic transitions among bottomonium (b-bbar) states other than the dipion transitions among upsns states. In our study of Y(3S) decays, we find a significant signal for Y(3S) ->…

High Energy Physics - Experiment · Physics 2007-05-23 D. Cronin-Hennessy , CLEO Collaboration

The Belle-II experiment is expected to collect large data samples at the $\Upsilon(4S)$ and $\Upsilon(5S)$ resonances to study primarily $B$ and $B_s$ mesons. We discuss what other data above the $B\bar{B}$ threshold are of interest. We…

High Energy Physics - Phenomenology · Physics 2017-03-08 A. E. Bondar , R. V. Mizuk , M. B. Voloshin

We suggest that the combined effect of screening, gluon-induced dissociation, collisional damping, and reduced feed-down explains most of the sequential suppression of Y(nS) states that has been observed in PbPb relative to pp collisions at…

High Energy Physics - Phenomenology · Physics 2012-07-27 Felix Nendzig , Georg Wolschin

We estimate the energy of the lowest Charmonium and Upsilon states with hybrid admixtures using the method of QCD Sum Rules. Our results show that the $\Psi'(2S)$ and $\Upsilon(3S)$ states both have about a 50% admixture of hybrid and meson…

High Energy Physics - Phenomenology · Physics 2009-07-09 Leonard S. Kisslinger

It is proposed that meson resonances are linear combinations of q-qbar and meson-meson (MM); baryon resonances are combinations of qqq and meson-baryon (MB). Mixing between these combinations arises via decays of confined states to…

High Energy Physics - Phenomenology · Physics 2010-05-19 D V Bugg

The Belle experiment at KEK accumulated a $121.4~{\rm fb}^{-1}$ sample of $e^+e^-$ collisions at the $\Upsilon(5S)$ resonance. This sample provides ample opportunity for improving the understanding of both the properties of $B_s$ mesons and…

High Energy Physics - Experiment · Physics 2013-12-06 Christian Oswald , Todd K. Pedlar

We study the processes $e^+e^-\to\omega\chi_{bJ}(1P)$ ($J$ = 0, 1, or 2) using samples at center-of-mass energies $\sqrt{s}$ = 10.701, 10.745, and 10.805 GeV, corresponding to 1.6, 9.8, and 4.7 fb$^{-1}$ of integrated luminosity,…

High Energy Physics - Experiment · Physics 2023-05-24 Belle II collaboration , I. Adachi , L. Aggarwal , H. Ahmed , H. Aihara , N. Akopov , A. Aloisio , N. Anh Ky , T. Aushev , V. Aushev , H. Bae , P. Bambade , Sw. Banerjee , J. Baudot , M. Bauer , A. Beaubien , J. Becker , P. K. Behera , J. V. Bennett , E. Bernieri , F. U. Bernlochner , V. Bertacchi , M. Bertemes , E. Bertholet , M. Bessner , S. Bettarini , B. Bhuyan , F. Bianchi , T. Bilka , D. Biswas , D. Bodrov , A. Bolz , A. Bondar , J. Borah , A. Bozek , M. Bracko , P. Branchini , T. E. Browder , A. Budano , S. Bussino , M. Campajola , L. Cao , G. Casarosa , C. Cecchi , M. -C. Chang , P. Cheema , V. Chekelian , Y. Q. Chen , K. Chilikin , K. Chirapatpimol , H. -E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , S. Choudhury , D. Cinabro , L. Corona , S. Cunliffe , S. Das , F. Dattola , E. De La Cruz-Burelo , S. A. De La Motte , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , M. Destefanis , S. Dey , A. De Yta-Hernandez , R. Dhamija , A. Di Canto , F. Di Capua , Z. Dolezal , I. Dominguez Jimenez , T. V. Dong , M. Dorigo , K. Dort , S. Dreyer , S. Dubey , G. Dujany , M. Eliachevitch , D. Epifanov , P. Feichtinger , T. Ferber , D. Ferlewicz , T. Fillinger , G. Finocchiaro , A. Fodor , F. Forti , B. G. Fulsom , E. Ganiev , A. Garmash , V. Gaur , A. Gaz , A. Gellrich , G. Ghevondyan , R. Giordano , A. Giri , A. Glazov , B. Gobbo , R. Godang , P. Goldenzweig , S. Granderath , E. Graziani , D. Greenwald , Z. Gruberova , T. Gu , Y. Guan , K. Gudkova , J. Guilliams , T. Hara , K. Hayasaka , H. Hayashii , S. Hazra , C. Hearty , I. Heredia de la Cruz , M. Hernandez Villanueva , A. Hershenhorn , T. Higuchi , E. C. Hill , H. Hirata , M. Hohmann , C. -L. Hsu , T. Iijima , K. Inami , G. Inguglia , N. Ipsita , A. Ishikawa , S. Ito , R. Itoh , M. Iwasaki , P. Jackson , W. W. Jacobs , D. E. Jaffe , E. -J. Jang , Q. P. Ji , S. Jia , Y. Jin , K. K. Joo , H. Junkerkalefeld , A. B. Kaliyar , K. H. Kang , R. Karl , G. Karyan , C. Ketter , C. Kiesling , C. -H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , H. Kindo , P. Kodys , T. Koga , S. Kohani , K. Kojima , T. Konno , A. Korobov , S. Korpar , E. Kovalenko , R. Kowalewski , T. M. G. Kraetzschmar , P. Krizan , P. Krokovny , R. Kumar , K. Kumara , T. Kunigo , A. Kuzmin , Y. -J. Kwon , S. Lacaprara , T. Lam , L. Lanceri , J. S. Lange , M. Laurenza , K. Lautenbach , R. Leboucher , P. M. Lewis , C. Li , L. K. Li , J. Libby , K. Lieret , Z. Liptak , Q. Y. Liu , D. Liventsev , S. Longo , A. Lozar , T. Lueck , C. Lyu , M. Maggiora , R. Maiti , R. Manfredi , E. Manoni , S. Marcello , C. Marinas , L. Martel , A. Martini , T. Martinov , L. Massaccesi , M. Masuda , K. Matsuoka , S. K. Maurya , J. A. McKenna , M. Merola , F. Metzner , M. Milesi , C. Miller , K. Miyabayashi , R. Mizuk , N. Molina-Gonzalez , S. Moneta , H. -G. Moser , M. Mrvar , R. Mussa , I. Nakamura , M. Nakao , Y. Nakazawa , A. Narimani Charan , M. Naruki , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , G. Nazaryan , N. K. Nisar , S. Ogawa , H. Ono , Y. Onuki , P. Oskin , A. Paladino , A. Panta , E. Paoloni , S. Pardi , H. Park , S. -H. Park , B. Paschen , A. Passeri , S. Paul , T. K. Pedlar , I. Peruzzi , R. Peschke , R. Pestotnik , M. Piccolo , L. E. Piilonen , P. L. M. Podesta-Lerma , T. Podobnik , S. Pokharel , L. Polat , C. Praz , S. Prell , E. Prencipe , M. T. Prim , H. Purwar , N. Rad , S. Raiz , A. Ramirez Morales , M. Reif , S. Reiter , M. Remnev , I. Ripp-Baudot , G. Rizzo , S. H. Robertson , J. M. Roney , A. Rostomyan , N. Rout , G. Russo , D. A. Sanders , S. Sandilya , A. Sangal , L. Santelj , Y. Sato , V. Savinov , B. Scavino , J. Schueler , C. Schwanda , Y. Seino , A. Selce , K. Senyo , J. Serrano , M. E. Sevior , C. Sfienti , C. P. Shen , X. D. Shi , T. Shillington , A. Sibidanov , J. B. Singh , J. Skorupa , R. J. Sobie , A. Soffer , E. Solovieva , S. Spataro , M. Staric , S. Stefkova , Z. S. Stottler , R. Stroili , Y. Sue , M. Sumihama , K. Sumisawa , W. Sutcliffe , S. Y. Suzuki , H. Svidras , M. Takizawa , U. Tamponi , K. Tanida , H. Tanigawa , F. Tenchini , A. Thaller , R. Tiwary , D. Tonelli , E. Torassa , N. Toutounji , K. Trabelsi , M. Uchida , I. Ueda , Y. Uematsu , T. Uglov , K. Unger , Y. Unno , K. Uno , S. Uno , Y. Ushiroda , S. E. Vahsen , R. van Tonder , G. S. Varner , A. Vinokurova , L. Vitale , V. Vobbilisetti , H. M. Wakeling , E. Wang , M. -Z. Wang , A. Warburton , S. Watanuki , M. Welsch , C. Wessel , E. Won , X. P. Xu , B. D. Yabsley , S. Yamada , W. Yan , S. B. Yang , H. Ye , J. Yelton , J. H. Yin , Y. M. Yook , K. Yoshihara , C. Z. Yuan , L. Zani , Y. Zhang , V. Zhilich , Q. D. Zhou , X. Y. Zhou , V. I. Zhukova , R. Zlebcik

Recently the Belle collaboration discovered two resonances, Zb(10610) and Zb(10650), that lie very close to the B\bar{B}^* and B^*\bar{B}^* thresholds, respectively. It is natural to suppose that these are molecular states of bottom and…

High Energy Physics - Phenomenology · Physics 2015-05-30 Thomas Mehen , Joshua W. Powell

Recent data from Belle show unusually large partial widths Upsilon(5S) --> Upsilon(1S) pi^+pi^- and \Upsilon(5S) --> \Upsilon(2S) pi^+ pi^-. The Z(4430) narrow resonance also reported by Belle in psi' pi^+ spectrum has the properties…

High Energy Physics - Phenomenology · Physics 2008-03-04 Marek Karliner , Harry J. Lipkin

The rates for magnetic dipole (M1) transitions $\Upsilon(nS) \to \eta_b(n'S) + \gamma$, $n' \le n$, are compared. The photon energies for allowed ($n' = n$) M1 transitions are very small, so hindered ($n' < n$) transitions could be more…

High Energy Physics - Phenomenology · Physics 2014-11-17 Stephen Godfrey , Jonathan L. Rosner

In this work, we study the isospin conserved hidden bottomonium decay of $X_b\to \Upsilon(1S)\omega$, where $X_b$ is taken to be the counterpart of the famous $X(3872)$ in the bottomonium sector as a candidate for the meson-meson molecule.…

High Energy Physics - Phenomenology · Physics 2015-06-23 Gang Li , Zhu Zhou