Search results for "Measurements of"

showing 10 items of 159 documents

Reconciling dark matter and solar neutrinos

1993

Abstract We present a simple model for neutrino dark matter in which neutrino masses arise radiatively and the solar neutrino data are explained via the MSW effect. The dark matter scale arises at the one-loop level with the MSW scale arises only in two loops. The model is compatible with all observational facts and allows observable ν e ν τ or ν μ ν τ oscillation rates in the laboratory if the limits from primordial big bang nucleosynthesis (BBN) are taken conservatively. In addition, it can be probed by searching for muon number violating processes such as μ → e + γ , and μ →3 e . These rates can well lie within the sensitivities of present experiments. Finally, if we ignore BBN limits we…

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoPhysics::Instrumentation and DetectorsSolar neutrinoDark matterHigh Energy Physics::PhenomenologyFísicaSolar neutrino problemNuclear physicsWarm dark matterMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationParticle Physics - Phenomenology
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Reconstructing Neutrino Properties from Collider Experiments in a Higgs Triplet Neutrino Mass Model

2003

We extend the minimal supersymmetric standard model with bilinear R-parity violation to include a pair of Higgs triplet superfields. The neutral components of the Higgs triplets develop small vacuum expectation values (VEVs) quadratic in the bilinear R-parity breaking parameters. In this scheme the atmospheric neutrino mass scale arises from bilinear R-parity breaking while for reasonable values of parameters the solar neutrino mass scale is generated from the small Higgs triplet VEVs. We calculate neutrino masses and mixing angles in this model and show how the model can be tested at future colliders. The branching ratios of the doubly charged triplet decays are related to the solar neutri…

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoSolar neutrinoHigh Energy Physics::PhenomenologyFísicaFOS: Physical scienceslaw.inventionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawHiggs bosonMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationColliderMinimal Supersymmetric Standard Model
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Light-neutrino mass spectrum, nuclear matrix elements, and the observability of neutrinoless ββ decay

2003

Parameters which describe neutrino flavor oscillations and neutrino mixing mechanisms, obtained from the analysis of the Sudbury Neutrino Observatory (SNO), Super-Kamiokande (SK), CHOOZ, KamLAND and WMAP data, are used to calculate upper limits of the effective neutrino mass 〈mν〉 relevant for the neutrinoless double-beta decay (0νββ). The observability of planned 0νββ experiments, and the present status of the decay of 76Ge are discussed within different light-neutrino mass spectra and by presenting a systematics on the available nuclear matrix elements.

PhysicsNuclear and High Energy PhysicsParticle physicsSudbury Neutrino ObservatoryPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoHigh Energy Physics::PhenomenologyCHOOZNuclear physicsDouble beta decayMass spectrumMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNuclear ExperimentNeutrino oscillationNuclear Physics A
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Detection of Atmospheric Muon Neutrinos with the IceCube 9-String Detector

2007

The IceCube neutrino detector is a cubic kilometer TeV to PeV neutrino detector under construction at the geographic South Pole. The dominant population of neutrinos detected in IceCube is due to meson decay in cosmic-ray air showers. These atmospheric neutrinos are relatively well understood and serve as a calibration and verification tool for the new detector. In 2006, the detector was approximately 10% completed, and we report on data acquired from the detector in this configuration. We observe an atmospheric neutrino signal consistent with expectations, demonstrating that the IceCube detector is capable of identifying neutrino events. In the first 137.4 days of live time, 234 neutrino c…

PhysicsNuclear and High Energy PhysicsParticle physicseducation.field_of_studyPhysics::Instrumentation and DetectorsPhysicsSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaPopulationDetectorAstrophysics (astro-ph)High Energy Physics::PhenomenologyAstrophysics::Instrumentation and Methods for AstrophysicsFOS: Physical sciencesSolar neutrino problemAstrophysicsNeutrino detectorAstronomiaMeasurements of neutrino speedddc:530High Energy Physics::ExperimentNeutrino astronomyNeutrinoeducation
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The response of (95,97)Mo to supernova neutrinos

2011

Knowledge about nuclear responses to neutrinos is essential for both astrophysical applications and studies of neutrino properties. We perform in this paper calculations of the cross sections for neutral-current neutrino scattering off the odd A = 95,97 Mo isotopes for energies appropriate for the detection of supernova neutrinos. Both the incoherent and coherent contributions to the cross sections are evaluated. The prominently contributing nuclear final states are identified and analysed. We employ the microscopic quasiparticle-phonon model (MQPM) to construct the wave functions of the initial and final nuclear states. The response of the aforementioned nuclei to supernova neutrinos are c…

PhysicsNuclear and High Energy PhysicsParticle physicsneutrino-nucleus scatteringIsotopedetectorAstrophysics::High Energy Astrophysical PhenomenaType II supernovamicroscopic quasiparticle-phonon modelNeutrino scatteringNuclear physicsCosmic neutrino backgroundSupernovaAbstract knowledgeMeasurements of neutrino speedmassNeutrinosupernova neutrinos
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Detecting the Diffuse Supernova Neutrino Background with LENA

2014

Low energy neutrino astronomy (LENA) has been proposed as a next generation 50 kt liquid scintillator detector. Its large target mass allows us to search for the diffuse supernova neutrino background (DSNB), which was generated by the cumulative emissions of all core-collapse supernovae throughout the Universe. Indistinguishable background from reactor and atmospheric electron antineutrinos limits the detection window to the energy range between 9.5 MeV and 25 MeV. Depending on the mean supernova neutrino energy, about 5 to 10 events per year are expected in this energy window. The background from neutral current reactions of atmospheric neutrinos surpasses the DSNB by more than one order m…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)Solar neutrino problemNuclear physicsSupernovaAstrophysics - Solar and Stellar AstrophysicsNeutrino detectorMeasurements of neutrino speedNeutrinoNeutrino astronomyAstrophysics - Instrumentation and Methods for AstrophysicsNeutrino oscillationInstrumentation and Methods for Astrophysics (astro-ph.IM)Solar and Stellar Astrophysics (astro-ph.SR)
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Results from the AMANDA neutrino telescope

2004

The Amanda neutrino telescope at the South Pole has been taking data since 1996. Stepwise upgraded, it reached its final stage in January 2000. We present results from the search for extraterrestrial neutrinos, neutrinos from dark matter annihilation and magnetic monopoles.

PhysicsNuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoHigh Energy Physics::PhenomenologyDark matterAstronomyAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsSolar neutrino problemAtomic and Molecular Physics and Opticslaw.inventionTelescopeNeutrino detectorlawMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino astronomyNeutrinoNuclear Physics B - Proceedings Supplements
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The Minimal 3 + 2 Neutrino Model vs. Higgs Decays

2016

Abstract The minimal 3+2 neutrino model is a Type-I seesaw model with two Weyl fermions, singlets under the Standard Model. Apart from light neutrino masses and mixings, this model can be fully described by four additional parameters. In this work, we study the minimal 3+2 neutrino model in scenarios where the singlets have masses at the GeV scale. This can lead to Higgs decays into heavy neutrinos, which could be observable as displaced vertices at the LHC.

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physics010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFermion01 natural sciencesStandard ModelSeesaw molecular geometry0103 physical sciencesHiggs bosonMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationNuclear and Particle Physics Proceedings
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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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