Abstract
Three hidden-charm pentaquark $P_c$ states, $P_c(4312)$, $P_c(4440)$ and
$P_c(4457)$ were revealed in the $Łambda_b^0J/p K^-$ process measured
by LHCb using both Run I and Run II data. Their nature is under lively
discussion, and their quantum numbers have not been determined. We analyze the
$J/\psi$ invariant mass distributions under the assumption that the
crossed-channel effects provide a smooth background. For the first time, such
an analysis is performed employing a coupled-channel formalism taking into
account heavy quark spin symmetry. We find that the data can be well described
in the hadronic molecular picture, which predicts seven $\Sigma_c^(*)\bar
D^(*)$ molecular states in two spin multiplets, such that the $P_c(4312)$ is
mainly a $\Sigma_cD$ bound state with $J^P=1/2^-$, while $P_c(4440)$ and
$P_c(4457)$ are $\Sigma_cD^*$ bound states with quantum numbers $3/2^-$
and $1/2^-$, respectively. We also show that there is clear evidence for a
narrow $\Sigma_c^*D$ bound state in the data which we call $P_c(4380)$,
different from the broad one reported by LHCb in 2015. With this state
established, all predicted $\Sigma_c D$, $\Sigma_c^* D$, and
$\Sigma_c D^*$ hadronic molecules are seen in the data, while the missing
three $\Sigma_c^*D^*$ states with smaller production rates are expected to
be found in future runs at the LHC or in photoproduction experiments.
Description
Evidence that the LHCb ${P_c}$ states are hadronic molecules and the existence of a narrow $P_c(4380)$
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