Search results for "Lepton"

showing 10 items of 1512 documents

The AMANDA neutrino detector - Status report

2000

Abstract The first stage of the AMANDA High Energy Neutrino Detector at the south Pole, the 302 PMT array AMANDA-B10, is taking data since 1997. We describe results on atmospheric neutrinos, limits on indirect WIMP detection, seasonal muon flux variation, relativistic monopole flux limits, a search for gravitational collapse neutrinos, and a depth scan of the optical ice properties. The next stage 19-string detector AMANDA-II with ∼650 PMTs will be completed in spring 2000.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaDetectorCosmic rayAtomic and Molecular Physics and OpticsParticle detectorMassless particleWIMPNeutrino detectorHigh Energy Physics::ExperimentNeutrinoLeptonNuclear Physics B - Proceedings Supplements
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17 keV neutrino in a singlet-triplet majoron model

1991

Abstract We investigate the possibility of a cosmologically safe 17 keV neutrino which may have been observed in the decays of tritium, S 35 , and C 14 within a singlet-triplet majoron model. Consideration of the leptonic decay of K + and X rays associated with the radiative decay of massive relic neutrinos severely constrains the scale of the spontaneous lepton number violation. It is argued that the mass density of relic 17 keV neutrinos is constrained as Ω v ⩽ 0.05 h −1 (0.01/ sin 2 θ ) in view of the observed diffuse X ray background.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyDark matterX-ray backgroundAstrophysics::Cosmology and Extragalactic AstrophysicsLepton numberCosmologyNuclear physicsHigh Energy Physics::ExperimentSinglet stateNeutrinoMajoronBosonPhysics Letters B
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On the nature of the fourth generation neutrino and its implications

2012

We consider the neutrino sector of a Standard Model with four generations. While the three light neutrinos can obtain their masses from a variety of mechanisms with or without new neutral fermions, fourth-generation neutrinos need at least one new relatively light right-handed neutrino. If lepton number is not conserved this neutrino must have a Majorana mass term whose size depends on the underlying mechanism for lepton number violation. Majorana masses for the fourth generation neutrinos induce relative large two-loop contributions to the light neutrino masses which could be even larger than the cosmological bounds. This sets strong limits on the mass parameters and mixings of the fourth …

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaFermionLepton numberStandard ModelMAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Fourth generationHigh Energy Physics::ExperimentNeutrino
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Working group on neutrino physics and astrophysics — concluding remarks I

1998

Abstract This part of the concluding remarks on the contributions and discussions in the working group on Neutrino Physics and Astrophysics summarises the following items: 1. 1) Neutrino mass measurement from Tritium beta decay, 2. 2) Neutrinoless double beta decay, 3. 3) Application of cryodetectors to the determination of neutrino properties, 4. 4) Search for a magnetic moment of the neutrino and, 5. 5) Limits on the mass of the Tau neutrino

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoHigh Energy Physics::PhenomenologyAstrophysicsSolar neutrino problemAtomic and Molecular Physics and OpticsNuclear physicsTau neutrinoDouble beta decayMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLeptonNuclear Physics B - Proceedings Supplements
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Fitting Simpson's neutrino into the standard model

1985

Abstract I show how to accomodate the 17 keV state recently reported by Simpson as one of the neutrinos of the standard model. Experimental constraints can only be satisfied if the μ and τ neutrino combine to a very good approximation to form a Dirac neutrino of 17 keV leaving a light ν e . Neutrino oscillations will provide the most stringent test of the model. The cosmological bounds are also satisfied in a natural way in models with Goldstone bosons. Explicit examples are given in the framework of majoron-type models. Constraints on the lepton symmetry breaking scale which follow from astrophysics, cosmology and laboratory experiments are discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsDirac (video compression format)Astrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFísicaStandard ModelGoldstone bosonMeasurements of neutrino speedHigh Energy Physics::ExperimentSymmetry breakingNeutrinoNeutrino oscillationParticle Physics - PhenomenologyLepton
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Superbeam studies at CERN

2003

Abstract A conventional low-energy neutrino beam of great intensity could be produced by the Super Proton Linac at CERN as a first stage of a Neutrino Factory. Water Cherenkov and liquid scintillator detectors are studied as possible candidates for a neutrino oscillation experiment which could improve our current knowledge of the atmospheric parameters Δmatm2, θ23 and measure or severely constrain θ13. It is also shown that a very large water detector could eventually observe leptonic CP violation.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFísicaSolar neutrino problemAccelerators and Storage RingsNuclear physicsNeutrino detectorCP violationPhysics::Accelerator PhysicsNeutrino FactoryHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationInstrumentationCherenkov radiationLepton
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Minimalistic Neutrino Mass Model

2000

We consider the simplest model which solves the solar and atmospheric neutrino puzzles, in the sense that it contains the smallest amount of beyond the Standard Model ingredients. The solar neutrino data is accounted for by Planck-mass effects while the atmospheric neutrino anomaly is due to the existence of a single right-handed neutrino at an intermediate mass scale between 10^9 GeV and 10^14 GeV. Even though the neutrino mixing angles are not exactly predicted, they can be naturally large, which agrees well with the current experimental situation. Furthermore, the amount of lepton asymmetry produced in the early universe by the decay of the right-handed neutrino is very predictive and ma…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoPhysics beyond the Standard Modelmedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAsymmetryUniverseHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoAnomaly (physics)BorexinoParticle Physics - PhenomenologyLeptonmedia_common
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Measurement ofK+production cross section by 8 GeV protons using high-energy neutrino interactions in the SciBooNE detector

2011

The SciBooNE Collaboration reports K+ production cross section and rate measurements using high energy daughter muon neutrino scattering data off the SciBar polystyrene (C8H8) target in the SciBooNE detector. The K+ mesons are produced by 8 GeV protons striking a beryllium target in Fermilab Booster Neutrino Beam line (BNB). Using observed neutrino and antineutrino events in SciBooNE, we measure d2σ/dpdΩ = (5.34 ±0.76) mb/(GeV/c x sr) for p + Be =K+ + X at mean K+ energy of 3.9 GeV and angle (with respect to the proton beam direction) of 3.7 degrees, corresponding to the selected K+ sample. Compared to Monte Carlo predictions using previous higher energy K+ production measurements, this mea…

PhysicsNuclear and High Energy PhysicsParticle physicsProtonMesonHadronNuclear physicsAntimatterHigh Energy Physics::ExperimentMuon neutrinoFermilabNeutrinoNuclear ExperimentLeptonPhysical Review D
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Measurement of the electron charge asymmetry inpp¯→W+X→eν+Xdecays inpp¯collisions ats=1.96  TeV

2015

We present a measurement of the electron charge asymmetry in $p\bar{p}\rightarrow W+X \rightarrow e\nu +X$ events at a center-of-mass energy of 1.96 TeV, using data corresponding to 9.7~fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider. The asymmetry is measured as a function of the electron pseudorapidity and is presented in five kinematic bins based on the electron transverse energy and the missing transverse energy in the event. The measured asymmetry is compared with next-to-leading-order predictions in perturbative quantum chromodynamics and provides accurate information for the determination of parton distribution functions of the prot…

PhysicsNuclear and High Energy PhysicsParticle physicsProtonmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronPartonElectron7. Clean energyAsymmetryNuclear physicsDistribution functionPseudorapidityHigh Energy Physics::ExperimentNuclear Experimentmedia_commonLeptonPhysical Review D
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Electromagnetism in nonleptonic weak interactions

2000

16 páginas, 1 figura.-- PACS: 11.30.Rd; 13.25.Es; 13.40.Ks.-- arXiv:hep-ph/0006172v2

PhysicsNuclear and High Energy PhysicsParticle physicsRenormalizationPhotonIsospin violationOrder (ring theory)FOS: Physical sciencesFísicaRenormalizationsymbols.namesakeTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)ElectromagnetismEffective lagrangiansChiral perturbation theorysymbolsEffective field theoryNonleptonic weak interactionsLagrangian
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