Search results for "neutrino physic"

showing 10 items of 70 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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A realistic model of neutrino masses with a large neutrinoless double beta decay rate

2011

The minimal Standard Model extension with the Weinberg operator does accommodate the observed neutrino masses and mixing, but predicts a neutrinoless double beta ($0\nu\beta\beta$) decay rate proportional to the effective electron neutrino mass, which can be then arbitrarily small within present experimental limits. However, in general $0\nu\beta\beta$ decay can have an independent origin and be near its present experimental bound; whereas neutrino masses are generated radiatively, contributing negligibly to $0\nu\beta\beta$ decay. We provide a realization of this scenario in a simple, well defined and testable model, with potential LHC effects and calculable neutrino masses, whose two-loop…

PhysicsNuclear and High Energy PhysicsParticle physicsHiggs PhysicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesType (model theory)Quantum numberPartícules (Física nuclear)Neutrino physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Standard-Model ExtensionDouble beta decayBeyond Standard ModelHigh Energy Physics::ExperimentConnection (algebraic framework)NeutrinoElectron neutrinoLepton
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Leptogenesis without violation of B-L

2009

We study the possibility of generating the observed baryon asymmetry via leptogenesis in the decay of heavy Standard Model singlet fermions which carry lepton number, in a framework without Majorana masses above the electroweak scale. Such scenario does not contain any source of total lepton number violation besides the Standard Model sphalerons, and the baryon asymmetry is generated by the interplay of lepton flavour effects and the sphaleron decoupling in the decay epoch.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaFermionLepton numberSphaleronHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryLeptogenesisBeyond Standard ModelHigh Energy Physics::ExperimentNeutrino PhysicsElectroweak scaleLepton
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Systematic decomposition of the neutrinoless double beta decay operator

2013

We discuss the systematic decomposition of the dimension nine neutrinoless double beta decay operator, focusing on mechanisms with potentially small contributions to neutrino mass, while being accessible at the LHC. We first provide a (d = 9 tree-level) complete list of diagrams for neutrinoless double beta decay. From this list one can easily recover all previously discussed contributions to the neutrinoless double beta decay process, such as the celebrated mass mechanism or "exotics", such as contributions from left-right symmetric models, R-parity violating supersymmetry and leptoquarks. More interestingly, however, we identify a number of new possibilities which have not been discussed …

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsOperator (physics)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetry01 natural sciencesBeta decayCosmologyHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesBeyond Standard ModelNeutrino PhysicsHigh Energy Physics::ExperimentNeutrino010306 general physics
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Performance of the NOMAD-STAR detector

2003

The NOMAD-STAR detector is a silicon vertex installed in the NOMAD spectrometer at the CERN SPS neutrino beam. It consists of four layers of a passive boron carbide target with a total mass of 45 kg and five layers of 600 single sided silicon microstrip detectors covering a total area of 1.14m^2. About 11,500 nu_mu charged current interactions were reconstructed in the fiducial volume of NOMAD-STAR from the neutrino run in 1998. The potential use of silicon detectors for nu_mu (nu_e) nu_tau oscillations depends on the observation of the tau candidates by the experimental signature of a large impact parameter, in the case of the one prong decay of the tau, or a double vertex, in the case of …

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSiliconSpectrometer010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsDetectorFísicachemistry.chemical_elementneutrino physics; silicon microstrip detectors01 natural sciencesNuclear physicschemistry0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentDetectors and Experimental TechniquesNeutrinoImpact parameter010306 general physicsInstrumentationCharged currentSTAR detector
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Sterile neutrinos with altered dispersion relations revisited

2020

In this paper we investigate neutrino oscillations with altered dispersion relations in the presence of sterile neutrinos. Modified dispersion relations represent an agnostic way to parameterize new physics. Models of this type have been suggested to explain global neutrino oscillation data, including deviations from the standard three-neutrino paradigm as observed by a few experiments. We show that, unfortunately, in this type of models new tensions arise turning them incompatible with global data.

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrino010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - Experiment3. Good healthHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Dispersion relationBeyond Standard Model0103 physical scienceslcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::Experiment010306 general physicsNeutrino oscillationJournal of High Energy Physics
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Fair scans of the seesaw. Consequences for predictions on LFV processes

2011

22 páginas, 5 figuras.-- El Pdf es la versión pre-print: arXiv:1010.5751v1

PhysicsNuclear and High Energy PhysicsParticle physicsSupersymmetric Standard Model010308 nuclear & particles physicsBranching fractionYukawa potentialFOS: Physical sciencesFísicaValue (computer science)Space (mathematics)01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Cover (topology)Seesaw molecular geometryLeptogenesis0103 physical sciencesNeutrino Physics010306 general physicsSimple (philosophy)Journal of High Energy Physics
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Non-standard neutrino oscillations: perspective from unitarity triangles

2021

We formulate an alternative approach based on unitarity triangles to describe neutrino oscillations in presence of non-standard interactions (NSI). Using perturbation theory, we derive the expression for the oscillation probability in case of NSI and cast it in terms of the three independent parameters of the leptonic unitarity triangle (LUT). The form invariance of the probability expression (even in presence of new physics scenario as long as the mixing matrix is unitary) facilitates a neat geometric view of neutrino oscillations in terms of LUT. We examine the regime of validity of perturbative expansions in the NSI case and make comparisons with approximate expressions existing in liter…

PhysicsNuclear and High Energy PhysicsUnitarity010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyDegrees of freedom (physics and chemistry)FOS: Physical sciencesQC770-798Invariant (physics)01 natural sciencesHigh Energy Physics - PhenomenologyTheoretical physicsMatrix (mathematics)CP violationHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. RadioactivityBeyond Standard Model0103 physical sciencesNeutrino PhysicsPerturbation theory (quantum mechanics)Neutrino010306 general physicsNeutrino oscillationJournal of High Energy Physics
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Effective Lagrangian approach to neutrinoless double beta decay and neutrino masses

2012

Neutrinoless double beta ($0\nu\beta\beta$) decay can in general produce electrons of either chirality, in contrast with the minimal Standard Model (SM) extension with only the addition of the Weinberg operator, which predicts two left-handed electrons in the final state. We classify the lepton number violating (LNV) effective operators with two leptons of either chirality but no quarks, ordered according to the magnitude of their contribution to \znbb decay. We point out that, for each of the three chirality assignments, $e_Le_L, e_Le_R$ and $e_Re_R$, there is only one LNV operator of the corresponding type to lowest order, and these have dimensions 5, 7 and 9, respectively. Neutrino masse…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaType (model theory)Lepton numberPartícules (Física nuclear)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Double beta decayBeyond Standard ModelNeutrino PhysicsHigh Energy Physics::ExperimentNeutrinoLepton
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Muon capture on light isotopes measured with the Double Chooz detector

2016

Using the Double Chooz detector, designed to measure the neutrino mixing angle $\theta_{13}$, the products of $\mu^-$ capture on $^{12}$C, $^{13}$C, $^{14}$N and $^{16}$O have been measured. Over a period of 489.5 days, $2.3\times10^6$ stopping cosmic $\mu^-$ have been collected, of which $1.8\times10^5$ captured on carbon, nitrogen, or oxygen nuclei in the inner detector scintillator or acrylic vessels. The resulting isotopes were tagged using prompt neutron emission (when applicable), the subsequent beta decays, and, in some cases, $\beta$-delayed neutrons. The most precise measurement of the rate of $^{12}\mathrm C(\mu^-,\nu)^{12}\mathrm B$ to date is reported: $6.57^{+0.11}_{-0.21}\time…

PhysicsSemileptonic decayParticle physicseducation.field_of_studyMuon010308 nuclear & particles physicsPopulationneutrino physic01 natural sciencesMuon captureNuclear physics13. Climate action0103 physical sciencesHigh Energy Physics::ExperimentNeutronProduction (computer science)Neutrino010306 general physicsGround stateeducation
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