The LHCb pentaquark as a $\bar{D}^*\Sigma_c-\bar{D}^*\Sigma_c^*$ molecular state

TL;DR

This paper provides a theoretical interpretation of the LHCb pentaquark as a molecular state composed mainly of D^*  and D^* ^* channels, matching experimental data on mass, width, and quantum numbers.

Contribution

It offers a detailed theoretical model explaining the pentaquark as a D^* -D^* ^* molecular state, supporting a specific quantum number assignment.

Findings

The model reproduces the experimental mass and width of the pentaquark.

The pentaquark is identified as a D^* -D^* ^* molecular state.

A D^* -D^* ^* composition explains the observed properties.

Abstract

We perform a theoretical analysis of the $\Lambda_b \to J/\psi K^- p$ reaction from where a recent LHCb experiment extracts a $\Lambda(1405)$ contribution in the $K^- p$ spectrum close to threshold and two baryon states of hidden charm in the $J/\psi\,p$ spectrum. We recall that baryon states of this type have been theoretically predicted matching the mass, width and $J^P$ of the experiment, concretely some states built up from the $J/\psi\, N$, $\bar D^* \Lambda_c$, $\bar D^* \Sigma_c$, $\bar D \Sigma^*_c$ and $\bar D^* \Sigma^*_c$ coupled channels. We assume that the observed narrow state around 4450 MeV has this nature and we are able to describe simultaneously the shapes and relative strength of the the $K^- p$ mass distribution close to threshold and the peak of the $J/\psi\,p$ distribution, with values of the $J/\psi\, p$ coupling to the resonance in line with the theoretical ones. The non trivial matching of many properties gives support to a $J^P=3/2^-$ assignment to this state and to its nature as a molecular state mostly made of $\bar D^* \Sigma_c$ and $\bar D^* \Sigma^*_c$.