Since the discovery of neutrino oscillations, the experimental progress in the last two decades has been very fast, with the precision measurements of the neutrino squared-mass differences and of the mixing angles, including the last unknown mixing angle θ 13 .Today a very large set of oscillation results obtained with a variety of experimental configurations and techniques can be interpreted in the framework of three active massive neutrinos, whose mass and flavour eigenstates are related by a 3 × 3 unitary mixing matrix, the Pontecorvo-Maki-Nakagawa-Sakata (PMNS) matrix, parameterized by three mixing angles θ 12 , θ 23 , θ 13 and a CP-violating phase δ CP . The additional parameters governing neutrino oscillations are the squaredmass differences ∆m 2 ji = m 2 j − m 2 i , where m i is the mass of the ith neutrino mass eigenstate. This review covers the rise of the PMNS three-neutrino mixing paradigm and the current status of the experimental determination of its parameters.The next years will continue to see a rich program of experimental endeavour coming to fruition and addressing the three missing pieces of the puzzle, namely the determination of the octant and precise value of the mixing angle θ 23 , the unveiling of the neutrino mass ordering (whether m 1 < m 2 < m 3 or m 3 < m 1 < m 2 ) and the measurement of the CP-violating phase δ CP .