Extended Data Fig. 2: Distributions of two-body and three-body masses of final-state particles.
From: Observation of charge–parity symmetry breaking in baryon decays

The mass distributions of (a) pK− and (b) π+π−, corresponding to the \({\Lambda }_{b}^{0}\to R(p{K}^{-})R({\pi }^{+}{\pi }^{-})\) phase-space region; (c) pπ− and (d) K−π+, corresponding to the \({\Lambda }_{b}^{0}\to R(p{\pi }^{-})R({K}^{-}{\pi }^{+})\) phase-space region; (e) pπ+π−, representing the \({\Lambda }_{b}^{0}\to R(p{\pi }^{+}{\pi }^{-}){K}^{-}\) phase-space region; and (f) K−π+π−, representing the \({\Lambda }_{b}^{0}\to R({K}^{-}{\pi }^{+}{\pi }^{-})p\) phase-space region. The \({\Lambda }_{b}^{0}\) and \({\bar{\Lambda }}_{b}^{0}\) samples are combined for the plots.