Study on the possible molecular states composed of $Λ_c\bar D^*$, $Σ_c\bar D^*$, $Ξ_c\bar D^*$ and $Ξ_c'\bar D^*$ in the Bethe-Salpeter frame based on the pentaquark states $P_c(4440)$, $P_c(4457)$ and $P_{cs}(4459)$ (2308.00582v2)
Abstract: The measurements on a few pentaquarks states $P_c(4440)$, $P_c(4457)$ and $P_{cs}(4459)$ excite our new interests about their structures. Since the masses of $P_c(4440)$ and $P_c(4457)$ are close to the threshold of $\Sigma_c\bar D*$, in the earlier works, they were regarded as molecular states of $\Sigma_c\bar D*$ with quantum numbers $I(JP)=\frac{1}{2}(\frac{1}{2}-)$ and $\frac{1}{2}(\frac{3}{2}-)$, respectively. In a similar way $P_{cs}(4459)$ is naturally considered as a $\Xi_c\bar D*$ bound state with $I=0$. Within the Bethe-Salpeter (B-S) framework we systematically study the possible bound states of $\Lambda_c\bar D*$, $\Sigma_c\bar D*$, $\Xi_c\bar D*$ and $\Xi_c'\bar D*$. Our results indicate that $\Sigma_c\bar D*$ can form a bound state with $I(JP)=\frac{1}{2}(\frac{1}{2}-)$, which corresponds to $P_c(4440)$. However for the $I(JP)=\frac{1}{2}(\frac{3}{2}-)$ system the attraction between $\Sigma_c$ and $\bar D*$ is too weak to constitute a molecule, so $P_{c}(4457)$ may not be a bound state of $\Sigma_c\bar D*$ with $I(JP)=\frac{1}{2}(\frac{3}{2}-)$. As $\Xi_c\bar D*$ and $\Xi_c'\bar D*$ systems we take into account of the mixing between $\Xi_c$ and $\Xi'c$ and the eigenstets should include two normal bound states $\Xi_c\bar D*$ and $\Xi_c'\bar D*$ with $I(JP)=\frac{1}{2}(\frac{1}{2}-)$ and a loosely bound state $\Xi_c\bar D*$ with $I(JP)=\frac{1}{2}(\frac{3}{2}-)$. The conclusion that two $\Xi_c\bar D*$ bound states exist, supports the suggestion that the observed peak of $P{cs}(4459)$ may hide two states $P_{cs}(4455)$ and $P_{cs}(4468)$. Based on the computations we predict a bound state $\Xi_c'\bar D*$ with $I(JP)=\frac{1}{2}(\frac{1}{2}-)$ but not that with $I(JP)=\frac{1}{2}(\frac{3}{2}-)$. Further more accurate experiments will test our approach and results.