Spectroscopy and decays of the fully-heavy tetraquarks

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作者
Muhammad Naeem Anwar
Jacopo Ferretti
Feng-Kun Guo
Elena Santopinto
Bing-Song Zou
机构
[1] Chinese Academy of Sciences,CAS Key Laboratory of Theoretical Physics, Institute of Theoretical Physics
[2] University of Chinese Academy of Sciences,Helmholtz
[3] Universität Bonn,Institut für Strahlen
[4] University of Chinese Academy of Sciences, und Kernphysik and Bethe Center for Theoretical Physics
[5] INFN,School of Physical Sciences
[6] Sezione di Genova,undefined
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We discuss the possible existence of the fully-heavy tetraquarks. We calculate the ground-state energy of the bbb¯b¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$bb {\bar{b}} {\bar{b}}$$\end{document} bound state, where b stands for the bottom quark, in a nonrelativistic effective field theory framework with one-gluon-exchange (OGE) color Coulomb interaction, and in a relativized diquark model characterized by OGE plus a confining potential. Our analysis advocates the existence of uni-flavor heavy four-quark bound states. The ground state bbb¯b¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$bb{\bar{b}}{\bar{b}}$$\end{document} tetraquark mass is predicted to be (18.72±0.02)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(18.72\pm 0.02)$$\end{document} GeV. Mass inequality relations among the lowest QQQ¯Q¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$QQ\bar{Q}\bar{Q}$$\end{document} states, where Q∈{c,b}\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q\in \{c, b\}$$\end{document}, and the corresponding heavy quarkonia are presented, which give the upper limit on the mass of ground state QQQ¯Q¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$QQ\bar{Q}\bar{Q}$$\end{document}. The possible decays of the lowest bbb¯b¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$bb\bar{b}\bar{b}$$\end{document} are highlighted, which might provide useful references in the search for them in ongoing LHC experiments, and its width is estimated to be a few tens of MeV.
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