Abstract. We discuss the possibility of reconstructing the neutrino mass spectrum from the complementary processes of neutrino oscillations and double beta decay in view of the new data of Super-Kamiokande presented at the Neutrino2000 conference. Since the large mixing angle solution is favored, now, the prospects to observe double beta decay and provide informations on the absolute mass scale in the neutrino sector have been improved.
Double Beta decay and neutrino oscillationsNeutrinos finally have been proven to be massive by atmospheric and solar neutrino oscillation experiments. However, the absolute scale of neutrino masses, a necessary ingredient for reconstructing beyond the standard model physics, is still unknown, since informations obtained in neutrino oscillation experiments regard the mass squared differences and mixing angles, only. Only both neutrino oscillations and neutrinoless double beta decay together could solve this absolute neutrino mass problem [1,2,3]. In this paper we discuss the most recent data , as presented by the Super-Kamiokande Collaboration at the Neutrino2000 conference [4]. The small mixing angle solution for solar neutrinos is ruled out, now, at 90 % C.L. Moreover, solutions including sterile neutrinos seemed to be disfavored both for atmospheric as well as for solar neutrinos. In the following we thus will restrict ourselves to a three neutrino framework, omitting the LSND anomaly. (For a discussion of the small mixing angle solution and four neutrino scenarios see [1]). A global analysis in a three neutrino framework yield the following favored regions [5,6]:• Solar neutrino oscillations favor ν e − ν e oscillations within the large mixing angle (LMA) MSW solution: ∆m 2 ⊙ = 3 (1 − 10) · 10 −5 eV 2 tan 2 θ ⊙ = 0.5 (0.2 − 0.6), where the bestfit is given with the 90 % C.L. region in the brackets. Also a small region in the QVO(quasi-vacuum-oscillation)-LOW regime at