Search results for "Seesaw molecular geometry"

showing 10 items of 89 documents

Minimal flavour seesaw models

2009

26 pages, 8 figures.-- ArXiv pre-print available at: http://arxiv.org/abs/0906.1461

PhysicsNuclear and High Energy PhysicsParticle physicsFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesInverseFísicaLepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometrySimple (abstract algebra)Beyond Standard ModelHigh Energy Physics::ExperimentNeutrino PhysicsNeutrinoMixing (physics)Lepton
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Neutrino anarchy and renormalization group evolution

2015

The observed pattern of neutrino mixing angles is in good agreement with the hypothesis of neutrino anarchy, which posits that Nature has chosen the entries of the leptonic mixing matrix at random. In this paper we investigate how stable this conclusion is under renormalization group effects. Working in the simplest type-I seesaw model and two variants of the inverse seesaw model we study how the statistical distributions of the neutrino mixing parameters evolve between the Grand Unification scale and the electroweak scale. Especially in the inverse seesaw case we find significant distortions: mixing angles tend to be smaller after RG running, and the Dirac CP phase tends to be closer to ze…

PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInverseFOS: Physical sciencesRenormalization group01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesProbability distributionGrand Unified TheoryNeutrinoElectroweak scale010306 general physicsPhysical Review D
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Inter-joint coordination of posture on a seesaw device

2016

Even though specific adjustments of the multi-joint control of posture have been observed when posture is challenged, multi-joint coordination on a seesaw device has never been accurately assessed. The current study was conducted in order to investigate the multi-joint coordination when subjects were standing on either a seesaw device or on a stable surface, with the eyes open or closed. Eighteen healthy active subjects were recruited. A principal component analysis and a Self-Organizing Maps analysis were performed on the joint angles in order to detect and characterize dominant coordination patterns. Intermuscular EMG coherence was analysed in order to assess the neurophysiological mechan…

AdultMaleComputer sciencePostureBiophysicsNeuroscience (miscellaneous)Postural control03 medical and health sciences0302 clinical medicineSeesaw molecular geometryControl theorymedicineHumansMuscle SkeletalPostural BalanceJoint (geology)Eyes openVision OcularPrincipal Component AnalysisProprioception030229 sport sciencesNeurophysiologymedicine.anatomical_structureFemaleNeurology (clinical)AnkleAnkleAnkle JointPsychomotor Performance030217 neurology & neurosurgeryCoherence (physics)Journal of Electromyography and Kinesiology
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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
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Top-seesaw assisted technicolor model with 126 GeV Higgs boson

2013

We discuss a model which involves the top quark condensation and the walking technicolor. We focus on the scalar boson in such a model from the viewpoint of the observed scalar boson at the LHC.

PhysicsCondensed Matter::Quantum GasesTop quarkParticle physicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorScalar bosonHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHiggs bosonHigh Energy Physics::ExperimentFocus (optics)
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Dynamical seesaw mechanism for Dirac neutrinos

2016

So far we have not been able to establish that, as theoretically expected, neutrinos are their own anti-particles. Here we propose a dynamical way to account for the Dirac nature of neutrinos and the smallness of their mass in terms of a new variant of the seesaw paradigm in which the energy scale of neutrino mass generation could be accessible to the current LHC experiments.

PhysicsParticle physicsNuclear and High Energy PhysicsCurrent (mathematics)Large Hadron Collider010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsDirac (video compression format)Mass generationHigh Energy Physics::PhenomenologyFOS: Physical sciencesNew variant01 natural scienceslcsh:QC1-999High Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicslcsh:PhysicsPhysics Letters B
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Nonunitary neutrino mixing in short and long-baseline experiments

2021

Non-unitary neutrino mixing in the light neutrino sector is a direct consequence of type-I seesaw neutrino mass models. In these models, light neutrino mixing is described by a sub-matrix of the full lepton mixing matrix and, then, it is not unitary in general. In consequence, neutrino oscillations are characterized by additional parameters, including new sources of CP violation. Here we perform a combined analysis of short and long-baseline neutrino oscillation data in this extended mixing scenario. We did not find a significant deviation from unitary mixing, and the complementary data sets have been used to constrain the non-unitarity parameters. We have also found that the T2K and NOvA t…

PhysicsParticle physicsPhysics::Instrumentation and DetectorsDirac (video compression format)Astrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesContext (language use)Unitary stateHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)
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Low-scale seesaw models versusNeff

2014

We consider the contribution of the extra sterile states in generic low-scale seesaw models to extra radiation, parametrized by ${N}_{\text{eff}}$. We find that the value of ${N}_{\text{eff}}$ is roughly independent of the seesaw scale within a wide range. We explore the full parameter space in the case of two extra sterile states and find that these models are strongly constrained by cosmological data for any value of the seesaw scale below $\mathcal{O}(100\text{ }\text{ }\mathrm{MeV})$.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaScale (descriptive set theory)Parameter space01 natural sciencesSeesaw molecular geometry0103 physical sciences010306 general physicsNeutrino oscillationPhysical Review D
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Minimal supersymmetric inverse seesaw: neutrino masses, lepton flavour violation and LHC phenomenology

2009

We study neutrino masses in the framework of the supersymmetric inverse seesaw model. Different from the non-supersymmetric version a minimal realization with just one pair of singlets is sufficient to explain all neutrino data. We compute the neutrino mass matrix up to 1-loop order and show how neutrino data can be described in terms of the model parameters. We then calculate rates for lepton flavour violating (LFV) processes, such as mu -> e gamma and chargino decays to singlet scalar neutrinos. The latter decays are potentially observable at the LHC and show a characteristic decay pattern dictated by the same parameters which generate the observed large neutrino angles.

Nuclear and High Energy PhysicsParticle physicsSupersymmetric Standard ModelPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)CharginoSeesaw molecular geometry0103 physical sciencesNeutrino Physics010306 general physicsParticle Physics - PhenomenologyPhysicsLarge Hadron Collider010308 nuclear & particles physicsRare DecaysHigh Energy Physics::PhenomenologyFísicaObservableMass matrixHigh Energy Physics - PhenomenologyBeyond Standard ModelHigh Energy Physics::ExperimentNeutrinoPhenomenology (particle physics)Lepton
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Minimal Supergravity Scalar Neutrino Dark Matter and Inverse Seesaw Neutrino Masses

2008

We show that within the inverse seesaw mechanism for generating neutrino masses minimal supergravity is more likely to have a sneutrino as the lightest superparticle than the conventional neutralino. We also demonstrate that such schemes naturally reconcile the small neutrino masses with the correct relic sneutrino dark matter abundance and accessible direct detection rates in nuclear recoil experiments.

Sterile neutrinoParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaDark matterGeneral Physics and AstronomyFOS: Physical sciencesAstrophysics01 natural sciences7. Clean energyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryastro-ph0103 physical sciences010306 general physicsNeutrino oscillationPhysics010308 nuclear & particles physicsSupergravityAstrophysics (astro-ph)High Energy Physics::PhenomenologyFísicahep-phSupersymmetryHigh Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics::ExperimentNeutrino
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