Search results for "seesaw mechanism"

showing 10 items of 56 documents

Supersymmetric mass spectra and the seesaw scale

2011

Supersymmetric mass spectra within two variants of the seesaw mechanism, commonly known as type-II and type-III seesaw, are calculated using full 2-loop RGEs and minimal Supergravity boundary conditions. The type-II seesaw is realized using one pair of 15 and $\bar{15}$ superfields, while the type-III is realized using three copies of $24_M$ superfields. Using published, estimated errors on SUSY mass observables attainable at the LHC and in a combined LHC+ILC analysis, we calculate expected errors for the parameters of the models, most notably the seesaw scale. If SUSY particles are within the reach of the ILC, pure mSugra can be distinguished from mSugra plus type-II or type-III seesaw for…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderScale (ratio)010308 nuclear & particles physicsSupergravityFOS: Physical sciencesFísicaObservableSupersymmetryParameter space01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSeesaw molecular geometry0103 physical sciences010306 general physics
researchProduct

Probing minimal supergravity in the type-I seesaw mechanism with lepton flavour violation at the CERN LHC

2008

The most general supersymmetric seesaw mechanism has too many parameters to be predictive and thus can not be excluded by any measurements of lepton flavour violating (LFV) processes. We focus on the simplest version of the type-I seesaw mechanism assuming minimal supergravity boundary conditions. We compute branching ratios for the LFV scalar tau decays, ${\tilde \tau}_2 \to (e,\mu) + \chi^0_1$, as well as loop-induced LFV decays at low energy, such as $l_i \to l_j + \gamma$ and $l_i \to 3 l_j$, exploring their sensitivity to the unknown seesaw parameters. We find some simple, extreme scenarios for the unknown right-handed parameters, where ratios of LFV branching ratios correlate with neu…

PhysicsNuclear and High Energy PhysicsParticle physicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetry7. Clean energy01 natural sciencesParticle decayHigh Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationLepton
researchProduct

Simplest scoto-seesaw mechanism

2019

By combining the simplest (3,1) version of the seesaw mechanism containing a single heavy "right-handed" neutrino with the minimal scotogenic approach to dark matter, we propose a theory for neutrino oscillations. The "atmospheric" mass scale arises at tree level from the seesaw, while the "solar" oscillation scale emerges radiatively, through a loop involving the "dark sector" exchange. Such simple setup gives a clear interpretation of the neutrino oscillation lengths, has a viable WIMP dark matter candidate, and implies a lower bound on the neutrinoless double beta decay rate.

PhysicsNuclear and High Energy PhysicsParticle physicsOscillationDark matterHigh Energy Physics::PhenomenologyFOS: Physical scienceslcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismWIMPSeesaw molecular geometryDouble beta decayHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationlcsh:Physics
researchProduct

Predicting charged lepton flavor violation from 3-3-1 gauge symmetry

2015

7 pages.- 2 figures.- v2: discussion extended

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismModelsHiggs bosonBosonStrong CP problemHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationPhenomenology (particle physics)Lepton
researchProduct

Testing neutrino mixing at future collider experiments

2000

Low energy supersymmetry with bilinear breaking of R-parity leads to a weak-scale seesaw mechanism for the atmospheric neutrino scale and a radiative mechanism for the solar neutrino scale. The model has striking implications for collider searches of supersymmetric particles. Assuming that the lightest SUSY particle is the lightest neutralino we demonstrate that (i) The neutralino decays inside the detector even for tiny neutrino masses. (ii) Measurements of the neutrino mixing angles lead to predictions for the ratios of various neutralino branching ratios implying an independent test of neutrino physics at future colliders, such as the Large Hadron Collider or a Linear Collider.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSolar neutrino problemLightest Supersymmetric Particlelaw.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Seesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)lawMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationColliderParticle Physics - Phenomenology
researchProduct

3-Neutrino Mass Spectrum from Combining Seesaw and Radiative Neutrino Mass Mechanisms

1999

We extend the Standard Model by adding a second Higgs doublet and a right-handed neutrino singlet with a heavy Majorana mass term. In this model, there are one heavy and three light Majorana neutrinos with a mass hierarchy m_3 >> m_2 >> m_1 such that that only m_3 is non-zero at the tree level and light because of the seesaw mechanism, m_2 is generated at the one-loop and m_1 at the two-loop level. We show that the atmospheric neutrino oscillations and large mixing MSW solar neutrino transitions with $��m^2_\mathrm{atm} \simeq m_3^2$ and $��m^2_\mathrm{solar} \simeq m_2^2$, respectively, are naturally accommodated in this model without employing any symmetry.

PhysicsNuclear and High Energy PhysicsParticle physicsSolar neutrinoHigh Energy Physics::PhenomenologyFOS: Physical sciencesStandard ModelMAJORANAHigh Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryMass spectrumHiggs bosonNeutrino
researchProduct

Leptogenesis with Single Right-Handed Neutrino Dominance

2001

We make an analytic and numerical study of leptogenesis in the framework of the (Supersymmetric) Standard Model plus the see-saw mechanism with a U(1) family symmetry and single right-handed neutrino dominance. In presenting our analytic and numerical results we make a clear distinction between the theoretically clean asymmetry parameter $\epsilon_1$ and the baryon asymmetry $Y_B$. In calculating $Y_B$ we propose and use a fit to the solutions to the Boltzmann equations which gives substantially more reliable results than parametrisations previously used in the literature. Our results show that there is a decoupling between the low energy neutrino observables and the leptogenesis prediction…

PhysicsNuclear and High Energy PhysicsParticle physicsSolar neutrinomedia_common.quotation_subjectHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesDecoupling (cosmology)AsymmetryHigh Energy Physics - PhenomenologyBaryon asymmetrySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)LeptogenesisNeutrinoNeutrino oscillationmedia_common
researchProduct

Flavour-symmetric type-II Dirac neutrino seesaw mechanism

2018

We propose a Standard Model extension with underlying A4 flavour symmetry where small Dirac neutrino masses arise from a Type-II seesaw mechanism. The model predicts the "golden" flavour-dependent bottom-tau mass relation, requires an inverted neutrino mass ordering and non-maximal atmospheric mixing angle. Using the latest neutrino oscillation global fit we derive restrictions on the oscillation parameters, such as a correlation between Dirac CP phase and the lightest neutrino mass.

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrino010308 nuclear & particles physicsOscillationDirac (video compression format)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesSymmetry (physics)lcsh:QC1-999High Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Standard-Model Extension0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationlcsh:PhysicsPhysics Letters B
researchProduct

New neutrino mass sum rule from the inverse seesaw mechanism

2012

A class of discrete flavor-symmetry-based models predicts constrained neutrino mass matrix schemes that lead to specific neutrino mass sum rules. One of these implies a lower bound on the effective neutrinoless double beta mass parameter, even for normal hierarchy neutrinos. Here we propose a new model based on the ${S}_{4}$ flavor symmetry that leads to the new neutrino mass sum rule and discuss how to generate a nonzero value for the reactor angle ${\ensuremath{\theta}}_{13}$ indicated by recent experiments, and the resulting correlation with the solar angle ${\ensuremath{\theta}}_{12}$.

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrino010308 nuclear & particles physicsSolar neutrinoHigh Energy Physics::PhenomenologyFísicaSolar neutrino problemMass matrix01 natural sciencesSeesaw mechanism0103 physical sciencesHigh Energy Physics::ExperimentSum rule in quantum mechanicsNeutrino010306 general physicsNeutrino oscillation
researchProduct

Inflation and majoron dark matter in the neutrino seesaw mechanism

2014

We propose that inflation and dark matter have a common origin, connected to the neutrino mass generation scheme. As a model we consider spontaneous breaking of global lepton number within the seesaw mechanism. We show that it provides an acceptable inflationary scenario consistent with the recent cosmic microwave background B-mode observation by the BICEP2 experiment. The scheme may also account for the baryon asymmetry of the Universe through leptogenesis for reasonable parameter choices.

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoDark matterHigh Energy Physics::PhenomenologyFísicaAstrophysics::Cosmology and Extragalactic AstrophysicsLepton numberSeesaw mechanismBaryon asymmetryLeptogenesisddc:530NeutrinoMajoron
researchProduct