Abstract
From the large-\(N_c\) QCD point of view, baryonia, tetraquark states, hybrids, and glueballs are studied. The existence of these states is argued for. They are constructed from baryons. In \(N_f=1\) large-\(N_c\) QCD, a baryonium is always identical to a glueball with \(N_c\) valence gluons. The ground state \(0^{-+}\) glueball has a mass of about 2450 MeV. \(f_0(1710)\) is identified as the lowest \(0^{++}\) glueball. The lowest four-quark nonet should be \(f_0(1370)\), \(a_0(1450)\), \(K^{\ast}_0(1430)\) and \(f_0(1500)\). Combining with the heavy quark effective theory, spectra of heavy baryonia and heavy tetraquark states are predicted. \(1/N_c\) corrections are discussed.
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12.39.Mk; 14.20.-c; 12.38.Lg
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Liu, C. Baryonium, tetraquark state and glueball in large-Nc QCD. Eur. Phys. J. C 53, 413–419 (2008). https://doi.org/10.1140/epjc/s10052-007-0471-8
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DOI: https://doi.org/10.1140/epjc/s10052-007-0471-8