Abstract.The two sources of MeV neutrinos, the Sun and the Supernovae are very interesting to study nowadays. Seismology aboard SoHO has properly constrained the solar emitted neutrino fluxes and consequently contributes to an unambiguous evidence of the solar neutrino oscillations. The main role of seismology stays nevertheless the description of the magneto-hydrodynamic processes and this progress provokes a renewal of the stellar discipline. Important results are noticed these three years, for the Sun. Future will be richer implying a large number of stars with an evident impact on supernovae and solar neutrino properties.
The Two Sources of N e u t r i n o sThe two natural Neutrino MeV Sources, the Sun and the Supernovae, are studied with more and more interest as the richness of their plasma properties is inaccessible in laboratories. Nevertheless, the level of knowledge of these sources is extremely different. The solar internal structure is scrutinized for twenty years with two independent probes: neutrinos and acoustic modes. In the case of supernovae, the emitted neutrinos have been detected once only, for the Supernova 1987A. It is evident that these two sources are extremely different. If the Sun has a continuous emission of neutrinos, the emission coming from a supernova explosion is quasi instantaneous, with a peak of 0.025 s. Only 6.4 % of the produced solar energy is emitted by the neutrinos, though the main part of the released energy in a supernova explosion is contained in the neutrino emission. If the Sun emits neutrinos up to 14 MeV and has a well determined energy spectrum, the range of emission for the supernovae is large from 5 MeV to about 100 MeV. The impact of the different neutrino oscillation solutions on the supernova energy spectrum is high, mainly for the SNO detector, even the waiting statistics in Superkamiokande is higher, so there is extremely large interest to detect supernova neutrinos in the present observatories to put more constraints on the neutrino properties or on the explosion mechanism. The diversity of the supernovae (Heger et al. 2003) and consequently of the supernova explosions encourages also the study of the different supernova precursors. Supernovae la have initial mass below 8 M©, and final mass probably below 1.5 M©, Supernovae II have initial mass between 8 to 30 M©, final mass below 10 M©, Supernovae lb and c have initial mass above 30 M© and final mass always below 10 M©. With such a range in mass, questions on geometry, asphericity, rotation, metallicity have not a clear answer today.The geometry of stars and the mass loss processes are more under control at different stages of evolution, so there is a renewal in stellar structure, which 9 terms of use, available at https://www.cambridge.org/core/terms. https://doi