2003/04/30 by F. R. Joaquim · 23 citations
Physics and Astronomy · #Anisotropy #Astrophysics and Cosmic Phenomena #CMB cold spot #Cosmic microwave background #Double beta decay #Neutrino #Neutrino Physics Research #Neutrino oscillation #Nuclear physics #Particle physics #Particle physics theoretical and experimental studies #Physics #Solar neutrino #Solar neutrino problem #hep-ph
paper · pdf · doi:10.1103/physrevd.68.033019
published in Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields 68(3) (American Physical Society) · Updated including the recent NC enhanced SNO data. Refferences added and typos corrected
openalex publication_date 2003/08/28 · arxiv created 2003/10/05 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
The first data released by the KamLAND Collaboration have confirmed the strong evidence in favor of the large mixing angle solution of the solar neutrino problem. Taking into account the ranges for the oscillation parameters allowed by the global analysis of the solar, CHOOZ and KamLAND data, we update the limits on the neutrinoless double beta decay effective neutrino mass parameter and analyze the impact of all the available data from neutrinoless double beta decay experiments on the neutrino mass bounds, in view of the latest WMAP results. For the normal neutrino mass spectrum the range (0.05--0.23) eV is obtained for the lightest neutrino mass if one takes into account the Heidelberg-Moscow evidence for neutrinoless double beta decay and the cosmological bound. It is also shown that under the same conditions the mass of the lightest neutrino may not be bounded from below if the spectrum is of the inverted type. Finally, we discuss how future experiments can improve the present bounds on the lightest neutrino mass set by the Troitsk, Mainz, and Wilkinson microwave anisotropy probe results.