The mass spectrum is studied with a data sample of collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 5.6 fb collected by the LHCb experiment. Three states are observed with a large significance and their masses and natural widths are measured to be \begin{eqnarray*} m(\Xi_c(2923)^0)&=& 2923.04 \pm 0.25 \pm 0.20 \pm 0.14 ~, \Gamma(\Xi_c(2923)^0) &=& 7.1 \pm 0.8 \pm 1.8 ~, \end{eqnarray*} \begin{eqnarray*} m(\Xi_c(2939)^0) &=& 2938.55 \pm 0.21 \pm 0.17 \pm 0.14 ~, \Gamma(\Xi_c(2939)^0) &=& 10.2 \pm 0.8 \pm 1.1 ~, \end{eqnarray*} \begin{eqnarray*} m(\Xi_c(2965)^0) &=& 2964.88 \pm 0.26 \pm 0.14 \pm 0.14~, \Gamma(\Xi_c(2965)^0) &=& 14.1 \pm 0.9 \pm 1.3~, \end{eqnarray*} where the uncertainties are statistical, systematic, and due to the limited knowledge of the mass. The and baryons are new states. The state is in the vicinity of the known baryon; however, their masses and natural widths differ significantly.

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