Charmonium-like states with the exotic quantum number \(J^{PC} = 3^{-+}\)
We apply the method of QCD sum rules to study the \(q c \bar q \bar c\) tetraquark states with the exotic quantum number \(J^{PC} = 3^{-+}\), and extract the mass of the lowest-lying state to be \({4.49^{+0.45}_{-0.41}}\) GeV. To construct the relevant tetraquark currents we need to explicitly add t...
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Published in | arXiv.org |
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Main Authors | , , , , , |
Format | Paper |
Language | English |
Published |
Ithaca
Cornell University Library, arXiv.org
19.10.2024
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Subjects | |
Online Access | Get full text |
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Summary: | We apply the method of QCD sum rules to study the \(q c \bar q \bar c\) tetraquark states with the exotic quantum number \(J^{PC} = 3^{-+}\), and extract the mass of the lowest-lying state to be \({4.49^{+0.45}_{-0.41}}\) GeV. To construct the relevant tetraquark currents we need to explicitly add the covariant derivative operator. Our systematic analysis of these interpolating currents indicates that: a) this state readily decays into the \(P\)-wave \([\rho J/\psi] / [\omega J/\psi ]\) channel but not into the \( [\rho \chi_{c2}]/[\omega \chi_{c2}]/[J/\psi f_2(1270)]\) channels, and b) it readily decays into the \([D^* \bar D_2^*]\) channel but not into the \(P\)-wave \([D^* \bar D^*]\) channel. |
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ISSN: | 2331-8422 |