Quantum Numbers of States and Other Charmed Baryons
arXiv:1704.00396 · doi:10.1103/PhysRevD.95.094018
Abstract
Possible spin-parity quantum numbers for excited charmed baryon resonances are discussed in this work. Our main results are: (i) Among the five newly observed states, we have identified and with radially excited and states, respectively, and with and . The two states and form a -wave doublet. (ii) The widths of and are calculable within the framework of heavy hadron chiral perturbation theory. (iii) Since the width of is of order 410 MeV, not all observed narrow baryons can be identified with states. (iv) For the antitriplet and states, their Regge trajectories for the orbital excitations of and are parallel to each other. Based on this nice property of parallelism, we see that the highest state does not fit if its quantum numbers are as found by LHCb. We suggest that is most likely the state. (v) The charmed baryon cannot be a state; otherwise, its width will be over 400~MeV, too large compared to the measured one. (vi) In the study of Regge trajectories of states, we find a missing state. It should have quantum numbers with a mass around 2920~MeV.
21 pages, 7 figures. Sec. II.A is substantially revised. Quantum number assignment to Omega_c(3050) and Omega_c(3066) is modified. Two more figures for the Regge trajectories in the (n_r, M^2) plane
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