Search results for "SEEs"

showing 10 items of 143 documents

Dark Matter and the elusive $\mathbf{Z'}$ in a dynamical Inverse Seesaw scenario

2017

The Inverse Seesaw naturally explains the smallness of neutrino masses via an approximate $B-L$ symmetry broken only by a correspondingly small parameter. In this work the possible dynamical generation of the Inverse Seesaw neutrino mass mechanism from the spontaneous breaking of a gauged $U(1)$ $B-L$ symmetry is investigated. Interestingly, the Inverse Seesaw pattern requires a chiral content such that anomaly cancellation predicts the existence of extra fermions belonging to a dark sector with large, non-trivial, charges under the $U(1)$ $B-L$. We investigate the phenomenology associated to these new states and find that one of them is a viable dark matter candidate with mass around the T…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSpontaneous symmetry breakingDark matterHigh Energy Physics::PhenomenologyInverseFOS: Physical sciencesFermion16. Peace & justice01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesBeyond Standard Modellcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrino010306 general physicsPhenomenology (particle physics)Boson
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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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Emotional Seesaw, Compliance, and Mindlessness

2001

Research on emotion conducted so far has ignored situations where the subject experiences a certain emotion, but where the external stimulus that evoked and upholds this emotion suddenly disappears. This kind of situation, however, is relatively common in everyday life. This article attempts to recognize certain consequences of those conditions under which the stimuli justifying our experience of such emotional states as fear or joy suddenly disappear. Research done to date by the author and colleagues indicates increased compliance of the subject when addressed with various requests, commands, or suggestions in the situation termed here “emotional seesaw.” The classical “live” example tha…

media_common.quotation_subjectStimulus (physiology)ObedienceArts and Humanities (miscellaneous)Seesaw molecular geometryInterrogationEveryday lifePsychologySocial psychologyGeneral PsychologyProbable mechanismCognitive psychologymedia_commonSocial influenceEuropean Psychologist
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Systematic study of the d=5 Weinberg operator at one-loop order

2012

We perform a systematic study of the $d=5$ Weinberg operator at the one-loop level. We identify three different categories of neutrino mass generation: (1) finite irreducible diagrams; (2) finite extensions of the usual seesaw mechanisms at one-loop and (3) divergent loop realizations of the seesaws. All radiative one-loop neutrino mass models must fall into one of these classes. Case (1) gives the leading contribution to neutrino mass naturally and a classic example of this class is the Zee model. We demonstrate that in order to prevent that a tree level contribution dominates in case (2), Majorana fermions running in the loop and an additional $\mathbb{Z}_2$ symmetry are needed for a genu…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsOperator (physics)Mass generationHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesCoupling (probability)01 natural sciencesLepton numberLoop (topology)MAJORANATheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesNeutrino010306 general physics
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Lepton Flavour Violation in charged leptons within SUSY-seesaw

2009

6 pages, 6 figures.-- Pre-print archive.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesContext (language use)SupersymmetryAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSeesaw molecular geometryHiggs bosonHigh Energy Physics::ExperimentNeutrinoLeptonMinimal Supersymmetric Standard Model
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Towards a New Minimal SO(10) Unification

2012

We argue that non-supersymmetric SO(10) models based on a renormalizable Higgs sector in which spontaneous symmetry breaking is triggered by the VEVs of a 45-dimensional adjoint and a 126-dimensional tensor representations can provide a potentially realistic yet relatively simple framework for a future robust estimate of the proton lifetime. Following closely the work Phys.Rev.D85, 095014 (2012), arXiv: 1202.0807 [hep-ph] we comment on the gauge unification constraints on the B-L breaking scale and show that there are several regions in the parameter space of the minimal model where the seesaw scale in the phenomenologically favoured ballpark of around 10^13-14 GeV is consistently supported.

PhysicsParticle physicsUnification010308 nuclear & particles physicsseesaw mechanismSpontaneous symmetry breakingbaryon and lepton number violationHigh Energy Physics::PhenomenologyFOS: Physical sciencesParameter spacebaryon and lepton number violation; proton decay; seesaw mechanism; SO(10) Grand Unification01 natural sciencesSO(10) Grand UnificationHiggs sectorMinimal modelproton decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesTensorSO(10)010306 general physics
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Leptogenesis with a dynamical seesaw scale

2014

In the simplest type-I seesaw leptogenesis scenario right-handed neutrino annihilation processes are absent. However, in the presence of new interactions these processes are possible and can affect the resulting $B-L$ asymmetry in an important way. A prominent example is provided by models with spontaneous lepton number violation, where the existence of new dynamical degrees of freedom can play a crucial role. In this context, we provide a model-independent discussion of the effects of right-handed neutrino annihilations. We show that in the weak washout regime, as long as the scattering processes remain slow compared with the Hubble expansion rate throughout the relevant temperature range,…

PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsmedia_common.quotation_subjectDegrees of freedom (statistics)FOS: Physical sciencesFísicaAstronomy and AstrophysicsContext (language use)01 natural sciencesLepton numberAsymmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryLeptogenesis0103 physical sciencesNeutrino010306 general physicsmedia_common
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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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Microbeam SEE Analysis of MIM Capacitors for GaN Amplifiers

2018

Broad-beam and microbeam single-event effect tests were performed on metal–insulator–metal capacitors with three different thicknesses of silicon nitride (Si3N4) dielectric insulator: 250, 500, and 750 nm. The broad-beam tests indicated that the devices with the thicker, 500- and 750-nm dielectric did not have a greater breakdown voltage. The surrounding structures of the capacitor were suspected to be a possible cause. Microbeam techniques made it possible to localize the failure location for the 500- and 750-nm devices. The failure occurs in the air bridge structure connected to the top capacitor plate, which can therefore be considered as an edge effect, while for the 250-nm devices, the…

Nuclear and High Energy PhysicsMaterials scienceInsulator (electricity)Dielectrickondensaattorit01 natural sciencesmetal–insulator–semiconductor (MIS) deviceslaw.inventionelektroniikkakomponentitchemistry.chemical_compoundlaw0103 physical sciencesBreakdown voltageElectrical and Electronic EngineeringMetal–insulator–metal (MIM) devicessingle event effects (SEEs)ta114ta213010308 nuclear & particles physicsbusiness.industryAmplifierMicrobeamsingle event gate ruptureCapacitorNuclear Energy and EngineeringSilicon nitridechemistrysäteilyfysiikkaElectrodeOptoelectronicsbusinessIEEE Transactions on Nuclear Science
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Minimal models with light sterile neutrinos

2011

We study the constraints imposed by neutrino oscillation experiments on the minimal extensions of the Standard Model (SM) with $n_R$ gauge singlet fermions ("right-handed neutrinos"), that can account for neutrino masses. We consider the most general coupling to SM fields of the new fields, in particular those that break lepton number and we do not assume any a priori hierarchy in the mass parameters. We proceed to analyze these models starting from the lowest level of complexity, defined by the number of extra fermionic degrees of freedom. The simplest choice that has enough free parameters in principle (i.e. two mass differences and two angles) to explain the confirmed solar and atmospher…

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physics010308 nuclear & particles physicsFOS: Physical sciencesFísica01 natural sciences7. Clean energyLepton numberStandard ModelMiniBooNEHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry13. Climate action0103 physical sciencesNeutrino010306 general physicsNeutrino oscillation
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