Search results for "Lepton"

showing 10 items of 1512 documents

Simultaneous analysis of neutrinoless double beta decay and LHC pp-cross sections: limits on the left-right mixing angle

2015

The extension of the Standard Model of electroweak interactions, to accommodate massive neutrinos and/or right-handed currents, is one of the fundamental questions to answer in the cross-field of particle and nuclear physics. The consequences of such extensions would reflect upon nuclear decays, like the very exotic nuclear double-beta-decay, as well as upon high-energy proton-proton reactions of the type performed at the LHC accelerator. In this talk we shall address this question by looking at the results reported by the ATLAS and CMS collaborations, where the excitation and decay of a heavy-mass boson may be mediated by a heavy-mass neutrino in proton-proton reactions leading to two jets…

PhysicsHistoryParticle physicsLarge Hadron ColliderElectroweak interactionNuclear TheoryHigh Energy Physics::PhenomenologyFísicaneutrinoless double beta decayComputer Science ApplicationsEducationStandard ModelNuclear physicsdouble-beta-decayDouble beta decayLHC acceleratorHigh Energy Physics::ExperimentLHCNeutrinoNuclear ExperimentMixing (physics)Ciencias ExactasLeptonBoson
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Long-Lived Slepton in the Coannihilation Region and Measurement of Lepton Flavour Violation at LHC

2009

When the mass difference between the lightest slepton and the lightest neutralino is smaller than the tau mass, the lifetime of the lightest slepton in the constrained Minimal Supersymmetric Standard Model (MSSM) increases in many orders of magnitude with respect to typical lifetimes of other supersymmetric particles. In a general MSSM, the lifetime of the lightest slepton is inversely proportional to the square of the intergenerational mixing in the slepton mass matrices. Such a long-lived slepton would produce a distinctive signature at LHC and a measurement of its lifetime would be relatively simple. Therefore, the long-lived slepton scenario offers an excellent opportunity to study lept…

PhysicsHistoryParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesComputer Science ApplicationsEducationHigh Energy Physics - Phenomenologymedicine.anatomical_structureHigh Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)Atlas (anatomy)NeutralinomedicineHigh Energy Physics::ExperimentMinimal Supersymmetric Standard ModelLepton
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Flavoured leptogenesis: A successful thermal leptogenesis withN1mass below 108GeV

2009

We prove that taking correctly into account the lepton flavour dependence of the CP asymmetries and washout processes, it is possible to obtain successful thermal leptogenesis from the decays of the second right-handed neutrino. The asymmetries in the muon and tau-flavour channels are then not erased by the inverse decays of the lightest right-handed neutrino, N1. In this way, we reopen the possibility of 'thermal leptogenesis' in models with a strong hierarchy in the right-handed Majorana masses that is typically the case in models with up-quark–neutrino Yukawa unification.

PhysicsHistoryParticle physicsMuonHierarchy (mathematics)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFlavourYukawa potentialComputer Science ApplicationsEducationMAJORANALeptogenesisHigh Energy Physics::ExperimentNeutrinoLeptonJournal of Physics: Conference Series
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An A4 model for neutrinos

2010

Proceedings of PASCOS 2010, the 16th International Symposium on Particles, Strings and Cosmology. 19 - 23 July 2010. Valencia (Spain)

PhysicsHistoryParticle physicsOperator (physics)High Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesScalar potentialComputer Science ApplicationsEducationHigh Energy Physics - PhenomenologyMAJORANAStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentNeutrinoLepton
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WIMPy baryogenesis with sterile neutrinos

2015

In this talk we propose a mechanism for baryogenesis from particle decays or annihilations that can work at the TeV scale. Some heavy particles annihilate or decay into a heavy sterile neutrino N (with M 1 TeV) and a "light" one ν (with m 100 GeV), generating an asymmetry among the two helicity degrees of freedom of v. This asymmetry is partially transferred to Standard Model leptons via fast Yukawa interactions and reprocessed into a baryon asymmetry by the electroweak sphalerons. We illustrate this mechanism in a WIMPy baryogenesis model where the helicity asymmetry is generated in the annihilation of dark matter. This model connects the baryon asymmetry, dark matter, and neutrino masses.

PhysicsHistoryParticle physicsSterile neutrinoAstrophysics::High Energy Astrophysical Phenomenamedia_common.quotation_subjectHigh Energy Physics::PhenomenologyDark matterElectroweak interactionAsymmetryComputer Science ApplicationsEducationBaryogenesisNuclear physicsBaryon asymmetryHigh Energy Physics::ExperimentNeutrinoLeptonmedia_commonJournal of Physics: Conference Series
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The calorimeter project for the Mu2e experiment

2013

The Mu2e experiment at Fermilab aims to measure the charged lepton flavor violating neutrinoless conversion of a negative muon into an electron. The conversion results in a monochromatic electron with an energy slightly below the rest mass of the muon (104.97 MeV). We expect to set a limit of ∼ 6×10^(−17) at 90% CL in three years of running, using an intense and clean pulsed μ^− beam providing ∼10^(18) stopped muons on target in three years of running. The experiment performs a strong suppression of potential background by gating off the prompts and performing precise momentum determination in conjunction with an highly efficient cosmic veto. The calorimeter should confirm that the candidat…

PhysicsLyso crystalNuclear and High Energy PhysicsParticle physicsPhotonMuonCalorimeter (particle physics)Mu2e experimentPhysics::Instrumentation and DetectorsElectronCalorimetryNuclear physicsMu2eHigh Energy Physics::ExperimentInvariant massFermilabInstrumentationLeptonNuclear and High Energy Physic
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Weak Interactions at Low Energy

1985

In this series of lectures, I would like to discuss the basic aspects of the standard electroweak theory, as well as some alternatives. The phenomenology associated with charged and neutral currents weak interaction will show the success of the standard theory in giving a quantitative account of the existing data. The framework of most of our considerations will be that of an effective theory at low momentum transfer, low with respect to the masses of the intermediate vector bosons, 80–90 GeV. As an extension of the standard theory for the leptonic sector, I will contemplate the possibility of massive neutrinos being described by Majorana fields, leading to exotic phenomena induced by lepto…

PhysicsMAJORANAParticle physicsHigh Energy Physics::PhenomenologyElectroweak interactionEffective field theoryHigh Energy Physics::ExperimentNeutrinoWeak interactionPhenomenology (particle physics)Lepton numberVector boson
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Electromagnetic properties of neutrinos in a background of electrons.

1989

Using covariant methods we calculate the neutrino electromagnetic vertex in a gas of electrons to lowest order in a loop expansion and to the lowest order in $\frac{1}{{M}_{W}^{2}}$. The new induced terms, while they are chirality preserving, yield additional contributions to the dipole moments in the nonrelativistic limit. These are identical for particles and antiparticles and so need not vanish for Majorana neutrinos. As applications of our formulas, the expression for the $\mathrm{plasmon}\ensuremath{\rightarrow}\ensuremath{\nu}\overline{\ensuremath{\nu}}$ decay rate is rederived and the dispersion relation of a massless neutrino propagating in matter in the presence of an external magn…

PhysicsMassless particleAntiparticleMAJORANAParticle physicsAntimatterQuantum mechanicsHigh Energy Physics::PhenomenologyElementary particleFermionNeutrinoLeptonPhysical review. D, Particles and fields
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Electromagnetic properties of neutrinos in a medium

1989

We show that, contrary to the situation in the vacuum, a Majorana neutrino can have electric and magnetic dipole moments in a medium. This is because of new contributions, equal for a particle and its antiparticle, that can arise only in a material background. For Dirac neutrinos, these contributions make the magnitudes of the dipole moments of the particle and the antiparticle unequal. We discuss the conditions which give rise to such effects, with particular attention to the role played by the discrete symmetries {ital C}, {ital P}, and {ital T}.

PhysicsMassless particleAntiparticleMAJORANAParticle physicsDipoleComputer Science::Information RetrievalHigh Energy Physics::ExperimentFermionNeutrinoMagnetic dipoleLeptonPhysical Review D
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Leptonic CP violation with massless neutrinos

1989

Abstract Leptonic CP violation may arise in the SU(2) ⊗ U(1) theory even if the neutrinos are strictly massless and, as a result, it is potentially large. Theoretical scenarios include isosinglet neutral heavy leptons which are present in many extensions of the standard electroweak theory such as superstring inspired models. We discuss in detail the nature of this CP violation and show that it can occur in a two-generation model. Possible effects are briefly discussed.

PhysicsMassless particleNuclear and High Energy PhysicsParticle physicsNeutral currentHigh Energy Physics::PhenomenologyElectroweak interactionCP violationSuperstring theoryHigh Energy Physics::ExperimentNeutrinoCharged currentLeptonPhysics Letters B
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