Search results for "Seesaw molecular geometry"

showing 10 items of 89 documents

Flavored CP asymmetries for type II seesaw leptogenesis

2013

A novel contribution to the leptonic CP asymmetries in type II seesaw leptogenesis scenarios is obtained for the cases in which flavor effects are relevant for the dynamics of leptogenesis. In the so-called flavored leptogenesis regime, the interference between the tree-level amplitude of the scalar triplet decaying into two leptons and the one-loop wave function correction with leptons in the loop, leads to a new nonvanishing CP asymmetry contribution. The latter conserves total lepton number but violates lepton flavor. Cases in which this novel contribution may be dominant in the generation of the baryon asymmetry are briefly discussed.

Nuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectFlavourScalar (mathematics)FOS: Physical sciences01 natural sciencesAsymmetryHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetrySeesaw molecular geometryModels0103 physical sciences010306 general physicsmedia_commonPhysicsViolation010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyBaryogenesisFísicaAstronomy and AstrophysicsNeutrino MassesLepton numberAtomic and Molecular Physics and OpticsTripletMixingsNeutrino physicsHigh Energy Physics - PhenomenologyGaugeLeptogenesisLeptogenesisSeesaw mechanismHigh Energy Physics::ExperimentLepton
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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
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The seesaw path to leptonic CP violation

2016

Future experiments such as SHiP and high-intensity $e^+ e^-$ colliders will have a superb sensitivity to heavy Majorana neutrinos with masses below $M_Z$. We show that the measurement of the mixing to electrons and muons of one such state could imply the discovery of leptonic CP violation in the context of seesaw models. We quantify in the minimal model the CP discovery potential of these future experiments, and demonstrate that a 5$\sigma$ CL discovery of leptonic CP violation would be possible in a very significant fraction of parameter space.

Particle physicsHeavy NeutrinoPhysics and Astronomy (miscellaneous)FOS: Physical sciencesSeesaw Modellcsh:AstrophysicsContext (language use)Parameter space01 natural sciencesMinimal modelHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometrySterile Neutrinolcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Particle Physics - PhenomenologyHeavy StatePhysicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyLight Neutrino Massehep-phHigh Energy Physics - PhenomenologyMAJORANAlcsh:QC770-798CP violationHigh Energy Physics::ExperimentNeutrino
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Majorana vs pseudo-Dirac neutrinos at the ILC

2019

Neutrino masses could originate in seesaw models testable at colliders, with light mediators and an approximate lepton number symmetry. The minimal model of this type contains two quasi-degenerate Majorana fermions forming a pseudo-Dirac pair. An important question is to what extent future colliders will have sensitivity to the splitting between the Majorana components, since this quantity signals the breaking of lepton number and is connected to the light neutrino masses. We consider the production of these neutral heavy leptons at the ILC, where their displaced decays provide a golden signal: a forward–backward charge asymmetry, which depends crucially on the mass splitting between the tw…

Particle physicsPhysics and Astronomy (miscellaneous)media_common.quotation_subjectFOS: Physical scienceslcsh:Astrophysics01 natural sciences7. Clean energyAsymmetryHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryDouble beta decay0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)media_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFermionLepton numberMAJORANAHigh Energy Physics - Phenomenologylcsh:QC770-798High Energy Physics::ExperimentNeutrinoLepton
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Gravity triggered neutrino condensates

2010

In this work we use the Schwinger-Dyson equations to study the possibility that an enhanced gravitational attraction triggers the formation of a right-handed neutrino condensate, inducing dynamical symmetry breaking and generating a Majorana mass for the right-handed neutrino at a scale appropriate for the seesaw mechanism. The composite field formed by the condensate phase could drive an early epoch of inflation. We find that to the lowest order, the theory does not allow dynamical symmetry breaking. Nevertheless, thanks to the large number of matter fields in the model, the suppression by additional powers in G of higher order terms can be compensated, boosting them up to their lowest ord…

PhysicsAstrofísicaNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Spontaneous symmetry breakingHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGravitationHigh Energy Physics - PhenomenologyExplicit symmetry breakingMAJORANASeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryNeutrinoAstrophysics - Cosmology and Nongalactic AstrophysicsLepton
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Composite Higgs bosons from neutrino condensates in an inverted see-saw scenario

2020

We present a realization of the idea that the Higgs boson is mainly a bound state of neutrinos induced by strong four-fermion interactions. The conflicts of this idea with the measured values of the top quark and Higgs boson masses are overcome by introducing, in addition to the right-handed neutrino, a new fermion singlet, which, at low energies, implements the inverse see-saw mechanism. The singlet fermions also develop a scalar bound state which mixes with the Higgs boson. This allows us to obtain a small Higgs boson mass even if the couplings are large, as required in composite scalar scenarios. The model gives the correct masses for the top quark and Higgs boson for compositeness scale…

PhysicsCondensed Matter::Quantum GasesTop quarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesFermion01 natural sciencesPartícules (Física nuclear)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentNeutrinoElectroweak scale010306 general physicsBoson
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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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Flavour and Collider Interplay for SUSY at LHC7

2011

The current 7 TeV run of the LHC experiment shall be able to probe gluino and squark masses up to values larger than 1 TeV. Assuming that hints for SUSY are found in the jets plus missing energy channel by the end of a 5 fb$^{-1}$ run, we explore the flavour constraints on three models with a CMSSM-like spectrum: the CMSSM itself, a Seesaw extension of the CMSSM, and Flavoured CMSSM. In particular, we focus on decays that might have been measured by the time the run is concluded, such as $B_s\to\mu\mu$ and $\mu\to e\gamma$. We also analyse constraints imposed by neutral meson bounds and electric dipole moments. The interplay between collider and flavour experiments is explored through the u…

PhysicsGluinoParticle physicsMissing energyLarge Hadron ColliderPhysics and Astronomy (miscellaneous)Meson010308 nuclear & particles physicsHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetry01 natural scienceslaw.inventionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometrylaw0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsColliderEngineering (miscellaneous)
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Seesaw scale, unification, and proton decay

2018

We investigate a simple realistic grand unified theory based on the $SU(5)$ gauge symmetry which predicts an upper bound on the proton decay lifetime for the channels $p \to K^+ \bar{\nu}$ and $p \to \pi^+ \bar{\nu}$, i.e. $\tau (p \to K^+ \bar{\nu}) \lesssim 3.4 \times 10^{35}$ and $\tau (p \to \pi^+ \bar{\nu}) \lesssim 1.7 \times 10^{34}$ years, respectively. In this context, the neutrino masses are generated through the type I and type III seesaw mechanisms, and one predicts that the field responsible for type III seesaw must be light with a mass below 500 TeV. We discuss the testability of this theory at current and future proton decay experiments.

PhysicsHigh Energy Physics - TheoryParticle physics010308 nuclear & particles physicsProton decayHigh Energy Physics::PhenomenologyFOS: Physical sciencesField (mathematics)Context (language use)Type (model theory)01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHigh Energy Physics - Theory (hep-th)0103 physical sciencesGrand Unified TheoryHigh Energy Physics::ExperimentNeutrino010306 general physicsGauge symmetry
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Right Handed Sneutrino Dark Matter in Inverse and Linear seesaw scenarios

2012

We consider supersymmetric models in which the right-handed sneutrino is a viable WIMP dark matter candidate. These are either simple extensions of the Minimal Supersymmetric Standard Model or models with the addition of an extra U(1) group. All of them can explain small neutrino masses, through either the Inverse or the Linear Seesaw mechanism. We investigate the properties of the dark matter candidate naturally arising in these scenarios. We check for phenomenological bounds, such as correct relic abundance, consistency with direct detection cross section limits and laboratory constraints. Especially, we comment on limitations of the model space due to lepton flavour violating charged lep…

PhysicsHistoryParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Dark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesSupersymmetryLightest Supersymmetric ParticleComputer Science ApplicationsEducationHigh Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHigh Energy Physics::ExperimentNeutrinoLeptonMinimal Supersymmetric Standard ModelAstrophysics - Cosmology and Nongalactic Astrophysics
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