Extended Data Fig. 6: Constraints on PMNS oscillation parameters in 1D and 2D for both orderings.
From: Joint neutrino oscillation analysis from the T2K and NOvA experiments
The 1D posterior probability distributions of \({\sin }^{2}2{\theta }_{13}\) (a), \({\sin }^{2}{\theta }_{23}\) (b), \(| \Delta {m}_{32}^{2}| \) (c), δCP (d), and corresponding 1σ, 2σ, 3σ 2D contours \({\sin }^{2}{\theta }_{23}-{\sin }^{2}2{\theta }_{13}\) (e), \(\Delta {m}_{32}^{2}-{\sin }^{2}{\theta }_{23}\) (f), \({\delta }_{{\rm{CP}}}-\Delta {m}_{32}^{2}\) (g), \(\Delta {m}_{32}^{2}-{\sin }^{2}2{\theta }_{13}\) (h), \({\delta }_{{\rm{CP}}}-{\sin }^{2}{\theta }_{23}\) (i), and \({\delta }_{{\rm{CP}}}-{\sin }^{2}2{\theta }_{13}\) (j) from the joint fit with reactor constraints marginalized over both mass orderings.
