Revisit assignments of the new excited $\Omega_c$ states with QCD sum rules
Eur. Phys. J. C77 (2017) 832 In this article, we distinguish the contributions of the positive parity and negative parity $\Omega_c$ states, study the masses and pole residues of the 1S, 1P, 2S and 2P $\Omega_c$ states with the spin $J=\frac{1}{2}$ and $\frac{3}{2}$ using the QCD sum rules in a cons...
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Main Authors | , , |
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Format | Journal Article |
Language | English |
Published |
28.06.2017
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Subjects | |
Online Access | Get full text |
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Summary: | Eur. Phys. J. C77 (2017) 832 In this article, we distinguish the contributions of the positive parity and
negative parity $\Omega_c$ states, study the masses and pole residues of the
1S, 1P, 2S and 2P $\Omega_c$ states with the spin $J=\frac{1}{2}$ and
$\frac{3}{2}$ using the QCD sum rules in a consistent way, and revisit the
assignments of the new narrow excited $\Omega_c^0$ states. The predictions
support assigning the $\Omega_c(3000)$ to be the 1P $\Omega_c$ state with
$J^P={\frac{1}{2}}^-$, assigning the $\Omega_c(3090)$ to be the 1P $\Omega_c$
state with $J^P={\frac{3}{2}}^-$ or the 2S $\Omega_c$ state with
$J^P={\frac{1}{2}}^+$, and assigning $\Omega_c(3119)$ to be the 2S $\Omega_c$
state with $J^P={\frac{3}{2}}^+$. |
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DOI: | 10.48550/arxiv.1706.09401 |