Search results for "NEUTRINO"

showing 10 items of 1752 documents

Falsifying high-scale baryogenesis with neutrinoless double beta decay and lepton flavor violation

2015

5 pages.- 2 figures

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Baryon asymmetryDouble beta decay0103 physical sciences010306 general physicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNon-conservationFísicaLepton numberSphaleron3. Good healthBaryogenesisHigh Energy Physics - PhenomenologyLeptogenesisLeptogenesisCP violationHigh Energy Physics::ExperimentNeutrino
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Flavour violation at the LHC: type-I versus type-II seesaw in minimal supergravity

2009

20 pages, 13 figures.-- ISI article identifier:000267789100003.-- ArXiv pre-print avaible at:http://arxiv.org/abs/0903.1408

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesNeutrino Physics010306 general physicsNeutrino oscillationPhysicsLarge Hadron Collider010308 nuclear & particles physicsSupergravityMass generationHigh Energy Physics::PhenomenologyFísicaRare decaysHigh Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics::ExperimentBeyond standard modelNeutrinoLeptonSupersymmetric standard model
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From transition magnetic moments to majorana neutrino masses

2005

It is well known that a majorana mass induces a (small) transition magnetic moment. The converse is also true; in this paper we estimate the loop contribution of transition magnetic moments $[\mu]_{\alpha \beta}$ to the neutrino mass matrix $[m]_{\alpha \beta}$. We show that for hierarchical neutrino masses, the contribution of $[\mu]_{e \tau}$ to $[m]_{e \tau}$ can exceed the experimental value of $[m]_{e \tau}$.

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciences01 natural sciencesNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesmental disorders010306 general physicsM-matrixPhysicsMagnetic moment010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaRenormalization groupMass matrixequipment and suppliesLoop (topology)MAJORANAHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]NeutrinoMass hierarchyhuman activities
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Constraining neutrinoless double beta decay

2011

A class of discrete flavor-symmetry-based models predicts constrained neutrino mass matrix schemes that lead to specific neutrino mass sum-rules (MSR). We show how these theories may constrain the absolute scale of neutrino mass, leading in most of the cases to a lower bound on the neutrinoless double beta decay effective amplitude.

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciences01 natural sciencesUpper and lower boundsHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNeutrino oscillationAbsolute scaleNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaMass matrixHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics::ExperimentNeutrino
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LHC signals of radiatively-induced neutrino masses and implications for the Zee-Babu model

2018

Contrary to the see-saw models, extended Higgs sectors leading to radiatively-induced neutrino masses do require the extra particles to be at the TeV scale. However, these new states have often exotic decays, to which experimental LHC searches performed so far, focused on scalars decaying into pairs of same-sign leptons, are not sensitive. In this paper we show that their experimental signatures can start to be tested with current LHC data if dedicated multi-region analyses correlating different observables are used. We also provide high-accuracy estimations of the complicated Standard Model backgrounds involved. For the case of the Zee-Babu model, we show that regions not yet constrained b…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesParameter space01 natural sciencesPartícules (Física nuclear)Higgs sectorStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenologylcsh:QC1-999High Energy Physics - PhenomenologyHiggs bosonHigh Energy Physics::ExperimentNeutrinolcsh:PhysicsLepton
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Determining Sneutrino Masses and Physical Implications

2005

In some areas of supersymmetry parameter space, sneutrinos are lighter than the charginos and the next-to-lightest neutralino, and they decay into the invisible neutrino plus lightest-neutralino channel with probability one. In such a scenario they can be searched for in decays of charginos that are pair-produced in e+e- collisions, and in associated sneutrino-chargino production in photon-electron collisions. The sneutrino properties can be determined with high accuracy from the edges of the decay energy spectra in the first case and from threshold scans in the second. In the final part of the report we investigate the mass difference of sneutrinos and charged sleptons between the third an…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesannihilation [electron positron]decay modes [chargino]SO(10) [grand unified theory]Nuclear physicsParticle decayHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometrypair production [chargino]interaction [photon electron]Invariant massddc:530numerical calculationsPhysicsmass difference [slepton]High Energy Physics::PhenomenologySuperpartnerSupersymmetryboundary conditionseesaw modelHigh Energy Physics - PhenomenologyPair productionNeutralino(4lepton 2sneutrino) [final state]width [chargino]branching ratio [chargino]High Energy Physics::Experimentassociated production [sneutrino]Neutrinomass spectrum [sneutrino]
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Searches for violation of lepton flavour and baryon number in tau lepton decays at LHCb

2013

Searches for the lepton flavour violating decay tau(-) -> mu(-)mu(+)mu(-) and the lepton flavour and baryon number violating decays tau(-) -> (p) over bar mu(+)mu(-) and tau(-) -> p mu(-)mu(-) have been carried out using proton-proton collision data, corresponding to an integrated luminosity of 1.0 fb(-1), taken by the LHCb experiment at root s = 7 TeV. No evidence has been found for any signal, and limits have been set at 90% confidence level on the branching fractions: B(tau(-) -> mu(-)mu(+)mu(-) mu(+)mu(-)) p mu(-)mu(-)) (p) over bar mu(+)mu(-) and tau(-) -> p mu(-)mu(-) decay modes represent the first direct experimental limits on these channels.

Nuclear and High Energy PhysicsParticle physicsFlavourDecays of leptons; Global symmetries (e.g. baryon number lepton number); 13.35.-r; 11.30.Fs;FOS: Physical sciences01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareNuclear physicslepton number)High Energy Physics - Experiment (hep-ex)Violació CP (Física nuclear)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]LHC flavour physics lepton number11.30.FsNeutrinsNeutrinos010306 general physicsParticles (Nuclear physics)Physics13.35.-rDecays of leptonsLarge Hadron Collider010308 nuclear & particles physicsGlobal symmetries (e.g. baryon number lepton number)Leptons (Física nuclear)Global symmetries (e.g.High Energy Physics::Phenomenologybaryon numberDecays of lepton3. Good healthFIS/01 - FISICA SPERIMENTALELeptons (Nuclear physics)Física nuclearHigh Energy Physics::ExperimentBaryon numberNeutrino11.30.FFIS/04 - FISICA NUCLEARE E SUBNUCLEAREParticle Physics - ExperimentLeptonCP violation (Nuclear physics)Physics Letters B
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A model of neutrino mass and dark matter with large neutrinoless double beta decay

2017

We propose a model where neutrino masses are generated at three loop order but neutrinoless double beta decay occurs at one loop. Thus we can have large neutrinoless double beta decay observable in the future experiments even when the neutrino masses are very small. The model receives strong constraints from the neutrino data and lepton flavor violating decays, which substantially reduces the number of free parameters. Our model also opens up the possibility of having several new scalars below the TeV regime, which can be explored at the collider experiments. Additionally, our model also has an unbroken $Z_2$ symmetry which allows us to identify a viable Dark Matter candidate.

Nuclear and High Energy PhysicsParticle physicsHiggs PhysicsDark matterFOS: Physical sciences01 natural scienceslaw.inventionHigh Energy Physics - Phenomenology (hep-ph)lawDouble beta decay0103 physical sciencesNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsColliderPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaObservableSymmetry (physics)High Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798High Energy Physics::ExperimentNeutrinoLeptonFree parameterJournal of High Energy Physics
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Novel mechanism for primordial perturbations in minimal extensions of the Standard Model

2020

Abstract We demonstrate that light spectator fields in their equilibrium can source sizeable CMB anisotropies through modulated reheating even in the absence of direct couplings to the inflaton. The effect arises when the phase space of the inflaton decay is modulated by the spectator which generates masses for the decay products. We call the mechanism indirect modulation and using the stochastic eigenvalue expansion show that it can source perturbations even four orders of magnitude larger than the observed amplitude. Importantly, the indirect mechanism is present in the Standard Model extended with right- handed neutrinos. For a minimally coupled Higgs boson this leads to a novel lower bo…

Nuclear and High Energy PhysicsParticle physicsHiggs Physicshiukkasfysiikka114 Physical sciences01 natural sciencesUpper and lower boundsPhysics Particles & FieldsStandard Model0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicscosmology of theories beyond the SM0206 Quantum PhysicsPhysicsScience & Technology0105 Mathematical Physics010308 nuclear & particles physicsHiggsin bosoniPhysicshep-thHigh Energy Physics::PhenomenologyHiggs physicshep-phInflatonCosmology of Theories beyond the SMNuclear & Particles PhysicsAmplitudeOrders of magnitude (time)Phase spacePhysical Sciences0202 Atomic Molecular Nuclear Particle and Plasma Physicsastro-ph.COHiggs bosonlcsh:QC770-798NeutrinoJournal of High Energy Physics
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Flavour in heavy neutrino searches at the LHC

2012

Heavy neutrinos at the TeV scale have been searched for at the LHC in the context of left-right models, under the assumption that they couple to the electron, the muon, or both. We show that current searches are also sensitive to heavy neutrinos coupling predominantly to the tau lepton, and present limits can significantly constrain the parameter space of general flavour mixing.

Nuclear and High Energy PhysicsParticle physicsLHC (Large Hadron Collider)Physics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHeavy neutrinoFOS: Physical sciencesContext (language use)ElectronParameter space01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsMixing (physics)PhysicsMuonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoLepton
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