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Related papers: Higher bottomonium zoo

200 papers

In the present work, we study the OZI-allowed three body open flavor decay properties of higher vector charmonium and bottomonium states with an extended quark pair creation model. For the bottomonium system, we get that (i) the $BB\pi$ and…

High Energy Physics - Phenomenology · Physics 2019-05-06 Xin-Zhen Weng , Li-Ye Xiao , Wei-Zhen Deng , Xiao-Lin Chen , Shi-Lin Zhu

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 coulomb plus linear (Cornell) potential is used to investigate the mass spectrum of bottomonium. Gaussian wave function is used in position and momentum space to estimate values of potential and kinetic energies, respectively. Based on…

High Energy Physics - Phenomenology · Physics 2022-01-28 Virendrasinh Kher , Raghav Chaturvedi , Nayneshkumar Devlani , A. K. Rai

In this article, we perform an systematic study of the radiative transitions among the bottomonium states based on the heavy quarkonium effective theory, and make predictions for the ratios among the radiative decay widths of a special…

High Energy Physics - Phenomenology · Physics 2012-10-30 Zhi-Gang Wang

The bottomonium mass spectra is computed in the framework of potential non-relativistic quantum chromodynamics. The potential consists of a static term incorporating Coulombic plus confinement part along with a correction term added…

High Energy Physics - Phenomenology · Physics 2022-01-05 Raghav Chaturvedi , Ajay Kumar Rai , Nakul R. Soni , Jignesh N. Pandya

The bottomonium states due to their varying binding energies dissolve at different temperatures and thus their nuclear modification factors and relative yields have potential to map the properties of Quark Gluon Plasma (QGP). We estimate…

High Energy Physics - Phenomenology · Physics 2015-06-11 A. Abdulsalam , Prashant Shukla

We study bottomonium production in heavy-ion collisions using a transport model which utilizes kinetic-rate and Boltzmann equations to calculate the energy, centrality and transverse-momentum ($p_T$) dependence of the yields. Both…

High Energy Physics - Phenomenology · Physics 2018-03-14 Xiaojian Du , Min He , Ralf Rapp

We review the most recent experimental progress in the hadron spectroscopy, up to bottomonium mass. This covers the search for the J^PC=1^-+ exotic state, the states in J/psi decays, the spin-singlets of heavy quarkonium, and the…

High Energy Physics - Experiment · Physics 2011-08-04 Chang-Zheng Yuan

Motivated by two news states $h_1(1911)$ and $X(2300)$ observed by BESIII, we have investigated the mass spectrum and the strong decay properties of the strangeonium mesons within the modified Godfrey-Isgur model by considering the…

High Energy Physics - Phenomenology · Physics 2025-08-26 Wei Hao , M. Atif Sultan , Li-Juan Liu , En Wang

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

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

Using samples of 102 million $\Upsilon(1S)$ and 158 million $\Upsilon(2S)$ events collected with the Belle detector, we study exclusive hadronic decays of these two bottomonium resonances to the three-body final states $\phi K^+ K^-$,…

High Energy Physics - Experiment · Physics 2012-08-16 Belle Collaboration , C. P. Shen , C. Z. Yuan , T. Iijima , I. Adachi , H. Aihara , D. M. Asner , T. Aushev , A. M. Bakich , A. Bay , K. Belous , B. Bhuyan , M. Bischofberger , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , M. -C. Chang , P. Chang , A. Chen , P. Chen , B. G. Cheon , K. Chilikin , R. Chistov , I. -S. Cho , K. Cho , S. -K. Choi , Y. Choi , J. Dalseno , Z. Doležal , Z. Drásal , S. Eidelman , J. E. Fast , V. Gaur , N. Gabyshev , Y. M. Goh , B. Golob , J. Haba , H. Hayashii , Y. Horii , Y. Hoshi , W. -S. Hou , Y. B. Hsiung , H. J. Hyun , K. Inami , A. Ishikawa , R. Itoh , M. Iwabuchi , Y. Iwasaki , T. Iwashita , T. Julius , J. H. Kang , T. Kawasaki , C. Kiesling , B. H. Kim , H. O. Kim , J. B. Kim , J. H. Kim , M. J. Kim , Y. J. Kim , K. Kinoshita , B. R. Ko , S. Koblitz , P. Kodyš , S. Korpar , R. T. Kouzes , P. Križan , P. Krokovny , R. Kumar , T. Kumita , A. Kuzmin , Y. -J. Kwon , S. -H. Lee , J. Li , Y. Li , J. Libby , C. Liu , Y. Liu , Z. Q. Liu , R. Louvot , S. McOnie , K. Miyabayashi , H. Miyata , G. B. Mohanty , D. Mohapatra , A. Moll , N. Muramatsu , E. Nakano , M. Nakao , Z. Natkaniec , S. Nishida , K. Nishimura , O. Nitoh , S. Ogawa , T. Ohshima , S. Okuno , S. L. Olsen , P. Pakhlov , G. Pakhlova , C. W. Park , H. Park , H. K. Park , T. K. Pedlar , R. Pestotnik , M. Petrič , L. E. Piilonen , M. Ritter , H. Sahoo , Y. Sakai , D. Santel , T. Sanuki , Y. Sato , O. Schneider , C. Schwanda , K. Senyo , O. Seon , M. E. Sevior , M. Shapkin , V. Shebalin , T. -A. Shibata , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , P. Smerkol , Y. -S. Sohn , A. Sokolov , E. Solovieva , M. Starič , M. Sumihama , T. Sumiyoshi , G. Tatishvili , Y. Teramoto , M. Uchida , S. Uehara , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Usov , P. Vanhoefer , G. Varner , C. H. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , K. M. Williams , E. Won , B. D. Yabsley , Y. Yamashita , C. C. Zhang , Z. P. Zhang , V. Zhilich , V. Zhulanov , A. Zupanc

We analyze the decays of the theoretically predicted lowest bottomonium hybrid $H(1P)$ to open bottom two-meson states. We do it by embedding a quark pair creation model into the Born-Oppenheimer framework which allows for a unified,…

High Energy Physics - Phenomenology · Physics 2021-01-26 Roberto Bruschini , Pedro González

The possibility to observe new bottomonium states with $J^{PC}= 1^{--}$ in the region $10.7-11.1$ GeV is discussed. The analysis of the di-electron widths shows that the $(n+1)^3S_1$ and $n^3D_1$ states ($n\geq 3$) may be mixed with a…

High Energy Physics - Phenomenology · Physics 2009-09-11 A. M. Badalian , B. L. G. Bakker , I. V. Danilkin

This paper gives results for the spectrum, all allowed E1 radiative partial widths (and some important M1 widths) and all open-charm strong decay amplitudes of all 40 c-cbar states expected up to the mass of the 4S multiplet, just above 4.4…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Barnes , S. Godfrey , E. S. Swanson

The mass modifications of the bottomonium states ($\Upsilon (NS)$,$N=1,2,3,4$ and $\Upsilon (1D)$) in magnetized nuclear matter are studied using chiral effective model. The in-medium masses are calculated from the medium modification of…

Nuclear Theory · Physics 2018-07-25 Amal Jahan C. S. , Shivam Kesarwani , Sushruth Reddy P. , Nikhil Dhale , Amruta Mishra

The shrinking of the bottomonium spectral function towards narrow quasi-particle states in a cooling strong-interaction medium at finite baryon density is followed within a holographic bottom-up model. The 5-dimensional…

High Energy Physics - Theory · Physics 2021-11-24 Rico Zöllner , Burkhard Kämpfer

We revisit the nonrelativistic quark model description of electromagnetic radiative decays in bottomonium. We show that even for the simplest spectroscopic quark model the calculated widths can be in good agreement with data once the…

High Energy Physics - Phenomenology · Physics 2020-01-09 R. Bruschini , P. González

The heavy quark spin symmetry implies that in addition to the recently observed Z(10610) and Z(10650) molecular resonances with $I^G=1^+$ there should exist two or four molecular bottomonium-like states with $I^G=1^-$. Properties of these…

High Energy Physics - Phenomenology · Physics 2013-05-29 M. B. Voloshin

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