Erratum: ${\mathrm{\Lambda }}_b\to J/\psi K\mathrm{\Xi }$ decay and the higher order chiral terms of the meson baryon interaction [Phys. Rev. D 92, 076015 (2015)]

Figure 1

Invariant mass distributions of $\pi \mathrm{\Sigma }$ and $\overline{K}N$ states in the decay modes ${\mathrm{\Lambda }}_b\to J/\psi \pi \mathrm{\Sigma }$ and ${\mathrm{\Lambda }}_b\to J/\psi \overline{K}N$, for the two models discussed in the text: model 1 (dashed lines) and model 2 (solid lines). The units in the $y$ axis are obtained taking $V_p=1$.

Figure 2

Invariant mass distributions of $K^{+}{\mathrm{\Xi }}^{-}$ states produced in the decay ${\mathrm{\Lambda }}_b\to J/\psi K^{+}{\mathrm{\Xi }}^{-}$, obtained for the two models discussed in the text: model 1 (dashed lines) and model 2 (solid lines). The thin lower lines correspond to omitting the next-to-leading-order (NLO) terms of the potential. The normalization is the same as in Fig. 1.

Figure 3

Invariant mass distributions of $\eta \mathrm{\Lambda }$ states produced in the decay ${\mathrm{\Lambda }}_b\to J/\psi \eta \mathrm{\Lambda }$, obtained for the two models discussed in the text: model 1 (dashed lines) and model 2 (solid lines). The thin lower lines correspond to omitting the NLO terms of the potential. The normalization is the same as in Fig. 4.

Figure 4

Comparison of the invariant mass distributions of $K^{+}{\mathrm{\Xi }}^{-}$ states (upper panel) and $\eta \mathrm{\Lambda }$ states (lower panel) obtained with model 1 (dashed lines) and model 2 (solid lines) with a pure phase-space distribution (dotted lines).