Spin-parities of the $P_c(4440)$ and $P_c(4457)$ in the One-Boson-Exchange Model

Abstract

The LHCb collaboration has recently observed three pentaquark peaks, the $P_c(4312)$, $P_c(4440)$ and $P_c(4457)$. They are very close to a pair of heavy baryon-meson thresholds, with the $P_c(4312)$ located $8.9\mathrm{MeV}$ below the $\bar{D}{\Sigma }_c$ threshold, and the $P_c(4440)$ and $P_c(4457)$ located $21.8$ and $4.8\mathrm{MeV}$ below the ${\bar{D}}^{\ast }{\Sigma }_c$ one. The spin-parities of these three states have not been measured yet. In this work we assume that the $P_c(4312)$ is a $J^P={\frac{1}{2}}^{-}$ $\bar{D}{\Sigma }_c$ bound state, while the $P_c(4440)$ and $P_c(4457)$ are ${\bar{D}}^{\ast }{\Sigma }_c$ bound states of unknown spin-parity, where we notice that the consistent description of the three pentaquarks in the one-boson-exchange model can indeed determine the spin and parities of the later, i.e. of the two ${\bar{D}}^{\ast }{\Sigma }_c$ molecular candidates. For this determination we revisit first the one-boson-exchange model, which in its original formulation contains a short-range delta-like contribution in the spin-spin component of the potential. We argue that it is better to remove these delta-like contributions because, in this way, the one-boson-exchange potential will comply with the naive expectation that the form factors should not have a significant impact in the long-range part of the potential (in particular the one-pion-exchange part). Once this is done, we find that it is possible to consistently describe the three pentaquarks, to the point that the $P_c(4440)$ and $P_c(4457)$ can be predicted from the $P_c(4312)$ within a couple of MeV with respect to their experimental location. In addition the so-constructed one-boson-exchange model predicts the preferred quantum numbers of the $P_c(4440)$ and $P_c(4457)$ molecular pentaquarks to be ${\frac{3}{2}}^{-}$ and ${\frac{1}{2}}^{-}$, respectively.

arXiv comment21 pages, 1 figure, 8 tables; discusses relation with EFT results; corresponds with published version

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• Magnetic moments and transition magnetic moments of $P_c$ and $P_{cs}$ states
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• Heavy-hadron molecular spectrum from light-meson exchange saturation
• Anticharmed strange pentaquarks from the one-boson-exchange model
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• Lattice QCD study of the elastic and transition form factors of charmed baryons
• Prompt production of the hidden charm pentaquarks in the LHC
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• Molecular pentaquark states with open charm and bottom flavors
• Possible molecular states from interactions of charmed baryons
• Insights into the nature of the $P_{cs}(4459)$