0000000000361994

AUTHOR

Josu Hernandez-garcia

showing 2 related works from this author

GeV-scale neutrinos: interactions with mesons and DUNE sensitivity

2021

The simplest extension of the SM to account for the observed neutrino masses and mixings is the addition of at least two singlet fermions (or right-handed neutrinos). If their masses lie at or below the GeV scale, such new fermions would be produced in meson decays. Similarly, provided they are sufficiently heavy, their decay channels may involve mesons in the final state. Although the couplings between mesons and heavy neutrinos have been computed previously, significant discrepancies can be found in the literature. The aim of this paper is to clarify such discrepancies and provide consistent expressions for all relevant effective operators involving mesons with masses up to 2 GeV. Moreove…

Particle physicsPhysics and Astronomy (miscellaneous)Scale (ratio)MesonFOS: Physical scienceslcsh:Astrophysics01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lcsh:QB460-4660103 physical sciencesDark Matterlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsDirac (video compression format)High Energy Physics::PhenomenologyFísicaFermionLeptonsHigh Energy Physics - PhenomenologyMAJORANAlcsh:QC770-798High Energy Physics::ExperimentNeutrinoNeutrino MassEvent (particle physics)Lepton
researchProduct

Global bounds on the Type-III Seesaw

2020

We derive general bounds on the Type-III Seesaw parameters from a global fit to flavor and electroweak precision data. We explore and compare three Type-III Seesaw realizations: a general scenario, where an arbitrary number of heavy triplets is integrated out without any further assumption, and the more constrained cases in which only 3 or 2 (minimal scenario) additional heavy states are included. The latter assumption implies rather non-trivial correlations in the Yukawa flavor structure of the model so as to reproduce the neutrino masses and mixings as measured in neutrino oscillations experiments and thus qualitative differences can be found with the more general scenario. In particular,…

Nuclear and High Energy PhysicsStructure (category theory)FOS: Physical sciencesType (model theory)01 natural sciencesPartícules (Física nuclear)Theoretical physicsOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsNeutrino oscillationPhysics010308 nuclear & particles physicsElectroweak interactionBeyond Standard Model; Neutrino PhysicsHigh Energy Physics::PhenomenologyYukawa potentialFísicaHigh Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798NeutrinoJournal of High Energy Physics
researchProduct