TY - JOUR
T1 - The electron neutrino mass, double beta decay and cosmology
AU - Langacker, Paul
AU - Sathiapalan, B.
AU - Steigman, Gary
N1 - Funding Information:
We are very gratefult o E. Kolb, D. Lindley, S. Nussinov,R . ScherrerM, . Turner and T. Walker for valuabled iscussionsa nd to J. Chauveaufo r communicatintgh e results of the CERN-PS-191 experimentT. his work was supportedin part by the Departmenot f Energy contractsE Y-76-C-02-3071(P .L. and B.S.) and DE-AC02-78ER-05007( G.S.). One of us (G.S.) would also like to thank the Theoretical AstrophysicsG roup at Fermilab for hospitalityw hile part of this work was done.
PY - 1986/3/24
Y1 - 1986/3/24
N2 - The Lubimov et al. experiment suggests a nonzero νe mass in the 20-45 eV range, while neutrinoless double beta decay experiments set upper limits between 2 and 10 eV if the νe is an unmixed Majorana particle. Together, these imply that the νe is either a Dirac neutrino or that it is a mixture of Majorana mass eigenstates which cancel in the double beta decay amplitude. We consider the laboratory and cosmological constraints on the latter possibility and show that it is ruled out except for two small regions of parameter space unless new physics is invoked to allow a fast invisible decay or annihilation channel for the heavy neutrino. Surprisingly, the cosmological constraints are often stronger if the heavy neutrino is mainly an SU2×U1 singlet than if it has normal weak interactions. Implications for the recently reported 17 keV neutrino are also discussed.
AB - The Lubimov et al. experiment suggests a nonzero νe mass in the 20-45 eV range, while neutrinoless double beta decay experiments set upper limits between 2 and 10 eV if the νe is an unmixed Majorana particle. Together, these imply that the νe is either a Dirac neutrino or that it is a mixture of Majorana mass eigenstates which cancel in the double beta decay amplitude. We consider the laboratory and cosmological constraints on the latter possibility and show that it is ruled out except for two small regions of parameter space unless new physics is invoked to allow a fast invisible decay or annihilation channel for the heavy neutrino. Surprisingly, the cosmological constraints are often stronger if the heavy neutrino is mainly an SU2×U1 singlet than if it has normal weak interactions. Implications for the recently reported 17 keV neutrino are also discussed.
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U2 - 10.1016/0550-3213(86)90191-4
DO - 10.1016/0550-3213(86)90191-4
M3 - Article
AN - SCOPUS:0010785298
SN - 0550-3213
VL - 266
SP - 669
EP - 686
JO - Nuclear Physics, Section B
JF - Nuclear Physics, Section B
IS - 3-4
ER -