Search results for "Lepton"

showing 10 items of 1512 documents

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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Neutrino Masses, Grand Unification, and Baryon Number Violation

2014

If grand unification is real, searches for baryon-number violation should be included on the list of observables that may reveal information regarding the origin of neutrino masses. Making use of an effective-operator approach and assuming that nature is SU(5) invariant at very short distances, we estimate the consequences of different scenarios that lead to light Majorana neutrinos for low-energy phenomena that violate baryon number minus lepton number (B-L) by two (or more) units, including neutron-antineutron oscillations and B-L violating nucleon decays. We find that, among all possible effective theories of lepton-number violation that lead to nonzero neutrino masses, only a subset is,…

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesLepton numberHigh Energy Physics - PhenomenologyMAJORANAGrand unification epochHigh Energy Physics - Phenomenology (hep-ph)Grand Unified TheoryHigh Energy Physics::ExperimentBaryon numberNeutrinoNeutrino oscillation
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Neutrino mixing and CP-violation

2000

The prospects of measuring the leptonic angles and CP-odd phases at a neutrino factory are discussed in two scenarios: 1) three active neutrinos as indicated by the present ensemble of atmospheric plus solar data; 2) three active plus one sterile neutrino when the LSND signal is also taken into account. For the latter we develop one and two mass dominance approximations. The appearance of wrong sign muons in long baseline experiments and tau leptons in short baseline ones provides the best tests of CP-violation in scenarios 1) and 2), respectively.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsMuonHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lcsh:QC770-798CP violationlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrino FactoryHigh Energy Physics::ExperimentNeutrinoMixing (physics)LeptonSign (mathematics)Particle Physics - Phenomenology
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ELECTROWEAK THEORY AND THE NEUTRINO-MASS AND NEUTRINO-OSCILLATION QUESTIONS

2007

It is shown that both conjectures of neutrino mass and neutrino oscillation can be made really well-grounded within the Standard Model provided that one adopts a recent new version of the electroweak scheme spontaneously giving also a fundamental explanation for the so-called "maximal parity-violation" effect. A crucial role is played by the prediction of two distinct, scalar and pseudoscalar, replicas of (electron, muon, and tau) lepton numbers that could fully account for an actual non-coincidence between neutrino mass-eigenstates and gauge-eigenstates.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsNeutrino oscillationNeutrino theory of lightHigh Energy Physics::PhenomenologyElectroweak interactionGeneral Physics and AstronomyAstronomy and AstrophysicsStandard Modelelementary-fermion masseMeasurements of neutrino speedHigh Energy Physics::Experimentmaximal parity-violation.NeutrinoNeutrino oscillationLepton
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Neutrino masses and mixing in A(4) models with three Higgs doublets

2013

We study neutrino masses and mixing in the context of flavor models with A(4) symmetry, three scalar doublets in the triplet representation, and three lepton families. We show that there is no representation assignment that yields a dimension-5 mass operator consistent with experiment. We then consider a type-I seesaw with three heavy right-handed neutrinos, explaining in detail why it fails, and allowing us to show that agreement with the present neutrino oscillation data can be recovered with the inclusion of dimension-3 heavy neutrino mass terms that break softly the A(4) symmetry.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsNeutrino theory of light010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyNon-conservationFOS: Physical sciencesFísicasymmetries01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationNon-ConservationLeptonSymmetries
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Leptogenesis with conservation of B–L

2012

Abstract We study leptogenesis in the decay of heavy Standard Model singlet fermions which carry lepton number, in a framework without Majorana masses above the electroweak scale. Based on M. C. Gonzalez-Garcia, J. Racker, N. Rius, JHEP 11 (2009) 079.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyLepton numberAtomic and Molecular Physics and OpticsStandard Model (mathematical formulation)MAJORANALeptogenesisHigh Energy Physics::ExperimentElectroweak scaleNeutrinoNuclear Physics B - Proceedings Supplements
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Physics at new accelerators: Looking beyond the Standard Model

1993

Abstract Neutrino masses can have important implications in nuclear and particle physics, astrophysics and cosmology. Apart from the effects related to solar neutrinos, neutrino oscillations, dark matter, beta and double beta decays, massive neutrinos can also produce signals in the new accelerators. Here I focus on μ and τ number violating processes, very promising for muon and tau factories, as well as on the signatures associated with spontaneously broken R parity supersymmetry and neutral heavy leptons. These include the possibility of high rates for single chargino and neutralino production at LEP, LHC/SSC, as well as new signatures involving invisibly decaying Higgs bosons.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelSolar neutrinoHigh Energy Physics::PhenomenologyFísicaSolar neutrino problemAtomic and Molecular Physics and OpticsNuclear physicsMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLeptonParticle Physics - Phenomenology
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Nucleosynthesis constraints on active-sterile neutrino conversions in the early universe with random magnetic field

1994

We consider active-sterile neutrino conversions in the early universe hot plasma in the presence of a random magnetic field generated at the electroweak phase transition. Within a random field domain the magnetization asymmetry of the lepton antilepton plasma produced by a uniform constant magnetic field is huge in contrast to their small density asymmetry, leading to a drastic change in the active-sterile conversion rates. Assuming that the random field provides the seed for the galactic field one can estimate the restrictions from primordial nucleosynthesis. Requiring that the extra sterile \neu does not enter in equilibrium with the active ones before nucleosynthesis we find limits of th…

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsRandom fieldField (physics)media_common.quotation_subjectHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaUniverseHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesisNucleosynthesisHigh Energy Physics::ExperimentNeutrinomedia_commonLeptonNuclear Physics B
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Reconciling neutrino anomalies in a simple four-neutrino scheme with R-parity violation

2000

We propose a simple extension of the MSSM based on extra compact dimensions which includes an $SU(2) \otimes U(1)$ singlet superfield. The fermion present in this superfield is the sterile neutrino, which combines with one linear combination of $\nu_e-\nu_{\mu}-\nu_{\tau}$ to form a Dirac pair whose mass accounts for the LSND anomaly. Its small mass can be ascribed to a volume suppression factor associated with extra compact dimensions. On the other hand the sterile neutrino scalar partner can trigger the spontaneous violation of R-parity, thereby inducing the necessary mass splittings to fit also the solar and atmospheric neutrino data. Thus the model can explain all neutrino oscillation d…

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaFermionLepton numberLightest Supersymmetric ParticleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-parityHigh Energy Physics::ExperimentNeutrinoNeutrino oscillation
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Measurement of the top quark mass in final states with two leptons

2009

We present measurements of the top quark mass in ttbar candidate events with two final state leptons using 1 inverse fb of data collected by the D0 experiment. Our data sample is selected by requiring two fully identified leptons or by relaxing one lepton requirement to an isolated track if at least one jet is tagged as a b jet. The top quark mass is extracted after reconstructing the event kinematics under the ttbar hypothesis using two methods. In the first method, we integrate over expected neutrino rapidity distributions, and in the second we calculate a weight for the possible top quark masses based on the observed particle momenta and the known parton distribution functions. We analyz…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyInverseFOS: Physical sciencesPartonJet (particle physics)D0 experiment7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RapidityHigh Energy Physics::ExperimentNeutrino010306 general physicsNuclear ExperimentLepton
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