Abstract. Since the first direct observations of antineutrino events by Reines and Cowan in the 1950's [1], nuclear reactors have been an important tool in the study of neutrino properties. More recently, the study of neutrino oscillations has been a very active area of research. The pioneering observation of oscillations by the KamLAND experiment has provided crucial information on the neutrino mixing matrix. New experiments to study the remaining unknown mixing angle are currently under development. These recent studies and potential future developments will be discussed. The standard model of particle physics contains (by hypothesis to reproduce the observed states) 3 generations of quarks and leptons. The quarks and charged leptons obtain their masses due to the Higgs mechanism, whereas the neutral leptons (neutrinos) are massless. The left-handed leptons belong to weak isospin doublets whereas the corresponding right-handed charged lepton IR is a weak isosinglet
KeywordsThe right-handed neutrinos do not appear in the standard model and there is no interaction that could generate such particles. The absence of the right-handed neutrino necessarily requires that niv = 0, since for niv ^0 a left-handed neutrino could become right-handed by a Lorentz transformation. It has been known for some time that, for the quarks, the mass eigenstates are not the same states as the flavor eigenstates produced in weak interactions. The flavor states are obtained by an SU(3) rotation of the mass eigenstates, described by a unitary rotation matrix known as the Cabibbo-Kobayashi-Maskawa (CKM) matrix. The CKM matrix is almost diagonal, and so it seems that there is some minor lack of alignment of the flavor and mass eigenstates. This slight rotation generates many interesting phenomena, including CP violation, but its origin is not understood at a fundamental level.During the last decade, we have obtained evidence for much stronger mixing of the neutrino flavor states [2]. This requires that neutrinos have finite mass, and implies that the mechanism for generating misalignment of the mass and flavor eigenstates is of greater importance than for the quarks. In particular, the strong mixing and much lighter values of neutrino mass (relative to the charged fermions) supports the view that neutrino