${\Lambda }_c(2910)$ and ${\Lambda }_c(2940)$ as the conventional baryons dressed with the $D^{\ast }N$ channel

Abstract

In this work, we treat ${\Lambda }_c(2910{)}^{+}$ and ${\Lambda }_c(2940{)}^{+}$ as the conventional $udc$ cores dressed with the $D^{\ast }N$ channel. We provide a possible interpretation to both ${\Lambda }_c(2910{)}^{+}$ and ${\Lambda }_c(2940{)}^{+}$ within the same framework. In the study, we consider not only the effects between the conventional triquark core and the $D^{\ast }N$ channel but also the $D^{\ast }N$-$D^{\ast }N$ interactions. The mass of ${\Lambda }_c$ state with $J^P=1/2^{-}$ is larger than that with $J^P=3/2^{-}$ in this unquenched picture, which is very different from the prediction of the conventional quenched quark model. Based on the mass spectrum, the spin-parity of ${\Lambda }_c(2940{)}^{+}$ is more likely to be $1/2^{-}$ while ${\Lambda }_c(2910{)}^{+}$ prefers $3/2^{-}$. We look forward to the future experiments can test our results with more precise experimental data.

arXiv comment12 pages, 4 tables, 5 figures

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