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WIMP dark matter as radiative neutrino mass messenger

A bstract The minimal seesaw extension of the Standard SU(3) c ⊗SU(2) L ⊗U(1) Y Model requires two electroweak singlet fermions in order to accommodate the neutrino oscillation parameters at tree level. Here we consider a next to minimal extension where light neutrino masses are generated radiativel...

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Published in:The journal of high energy physics 2013-10, Vol.2013 (10), p.1-18, Article 149
Main Authors: Hirsch, M., Lineros, R. A., Morisi, S., Palacio, J., Rojas, N., Valle, J. W. F.
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cited_by cdi_FETCH-LOGICAL-c343t-90cb183bb3180e9a74579b454ef592d77827464f8179338029e167e2359314333
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description A bstract The minimal seesaw extension of the Standard SU(3) c ⊗SU(2) L ⊗U(1) Y Model requires two electroweak singlet fermions in order to accommodate the neutrino oscillation parameters at tree level. Here we consider a next to minimal extension where light neutrino masses are generated radiatively by two electroweak fermions: one singlet and one triplet under SU(2) L . These should be odd under a parity symmetry and their mixing gives rise to a stable weakly interactive massive particle (WIMP) dark matter candidate. For mass in the GeV-TeV range, it reproduces the correct relic density, and provides an observable signal in nuclear recoil direct detection experiments. The fermion triplet component of the dark matter has gauge interactions, making it also detectable at present and near future collider experiments.
doi_str_mv 10.1007/JHEP10(2013)149
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subjects Classical and Quantum Gravitation
Dark matter
Density
Elementary Particles
Fermions
High energy physics
Interactive
Neutrinos
Oscillations
Physics
Physics and Astronomy
Quantum Field Theories
Quantum Field Theory
Quantum Physics
Recoil
Relativity Theory
String Theory
title WIMP dark matter as radiative neutrino mass messenger
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