Search results for "Instrumentation"

showing 10 items of 4914 documents

Reconciling dark matter, solar and atmospheric neutrinos

1993

We present models that can reconcile the solar and atmospheric neutrino data with the existence of a hot dark matter component in the universe. This dark matter is a quasi-Dirac neutrino whose mass $m_{DM}$ arises at the one-loop level. The solar neutrino deficit is explained via nonadiabatic conversions of electron neutrino to a sterile neutrino and the atmospheric neutrino data via maximal muon neutrino to tau neutrino oscillations generated by higher order loop diagrams. For $m_{DM} \sim 30$ eV the radiative neutrino decay can lead to photons that can ionize interstellar hydrogen. In one of the models one can have observable $\nu_e$ to $\nu_\tau$ oscillation rates, with no appreciable mu…

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoMuonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoHot dark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Tau neutrinoHigh Energy Physics::ExperimentMuon neutrinoNeutrinoElectron neutrinoComputer Science::DatabasesNuclear Physics B
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Neutrino masses and cosmology: current bounds and future sensitivities

2005

After a short introduction on the predicted cosmic neutrino background, we review the connection between neutrino masses and cosmology. We show how a combined analysis of data from the anisotropies of the cosmic microwave background radiation and from the distribution of cosmological large-scale structure gives a bound on the sum of neutrino masses. We briefly discuss the sensitivity of future cosmological data to neutrino masses.

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoHigh Energy Physics::PhenomenologyAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsSolar neutrino problemAtomic and Molecular Physics and OpticsCosmic neutrino backgroundMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino astronomyNeutrinoNeutrino oscillationNuclear Physics B - Proceedings Supplements
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Four species neutrino oscillations at nu-Factory: sensitivity and CP-violation

1999

The prospects of measuring the leptonic angles and CP-odd phases at a {\em neutrino factory} are discussed in the scenario of three active plus one sterile neutrino. We consider the $\nu_\mu \raw \nu_e$ LSND signal. Its associated large mass difference leads to observable neutrino oscillations at short ($\sim 1$ km) baseline experiments. Sensitivities to the leptonic angles down to $10^{-3}$ can be easily achieved with a 1 Ton detector. Longer baseline experiments ($\sim 100$ km) with a 1 Kton detector can provide very clean tests of CP-violation especially through tau lepton detection.

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoPhysics::Instrumentation and DetectorsDetectorHigh Energy Physics::PhenomenologyFísicaObservableHigh Energy Physics - PhenomenologyCP violationNeutrino FactoryHigh Energy Physics::ExperimentSensitivity (control systems)Neutrino oscillationInstrumentationLeptonParticle Physics - Phenomenology
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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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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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Cosmic Ray Results from the CosmoALEPH Experiment

2008

CosmoALEPH is an experiment operated in conjunction with the ALEPH detector. The ALEPH experiment took data from 1989 until the year 2000 at the Large Electron Positron Collider (LEP) at CERN. It provides, among others, high resolution tracking and calorimetry. CosmoALEPH used this e + e − detector for cosmic ray studies. In addition, six scintillator telescopes were installed in the ALEPH pit and the LEP tunnel. The whole experiment operated underground at a vertical depth of 320 meter water equivalent. Data from ALEPH and the scintillator telescopes provide informaton on the lateral distribution of energetic cosmic ray muons in extensive air showers. The decoherence curve of these remnant…

PhysicsNuclear and High Energy PhysicsParticle physicsTime projection chamberLarge Hadron ColliderMuonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaAstrophysics::Instrumentation and Methods for AstrophysicsCosmic rayAtomic and Molecular Physics and OpticsNuclear physicsAir showerLarge Electron–Positron ColliderHigh Energy Physics::ExperimentALEPH experimentMeter water equivalentNuclear Physics B - Proceedings Supplements
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The cosmic ray muon spectrum and charge ratio in CosmoALEPH

2004

Abstract The ALEPH experiment at the LEP e+e− storage ring at CERN has been used to measure the momentum spectrum of cosmic ray muons. ALEPH is located at a vertical depth of 320 m.w.e. underground close to the Jura mountains. The high resolution of the time projection chamber (TPC) of ALEPH allows to reconstruct muon tracks with momenta up to the TeV region. The measured muon momentum spectrum and the charge ratio in the range from 80 to 2500 GeV are presented. After corrections for energy loss in the overburden the sea level muon spectrum at nearly vertical incidence is obtained. The experimental data are compared to theoretical expectations and results from other experiments.

PhysicsNuclear and High Energy PhysicsParticle physicsTime projection chamberLarge Hadron ColliderMuonPhysics::Instrumentation and DetectorsCosmic rayNuclear physicsMomentumMuon colliderPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentInstrumentationALEPH experimentStorage ringNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Future experiments on hypernuclei and hyperatoms

2004

Abstract The possibility to produce double Λ nuclei in anti-proton nucleus collisions at anti-proton momenta close to the threshold for Ξ − Ξ + is explored. Combining a high-luminosity antiproton beam with a novel solid-state tracking system and a high-rate Ge-array, γ-spectroscopy of ΛΛ-hypernuclei will become feasible at the PANDA experiment of the future International Accelerator Facility at GSI.

PhysicsNuclear and High Energy PhysicsParticle physicsbusiness.industryNuclear TheoryTracking systemNuclear physicsmedicine.anatomical_structureAntiproton beamAntiprotonmedicinePhysics::Accelerator PhysicsNuclear ExperimentbusinessInstrumentationNucleusNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Kalman filter tracking and vertexing in a silicon detector for neutrino physics

2002

Abstract This article describes the application of Kalman filter techniques for the tracking and vertexing of particles inside the NOMAD-STAR detector, a silicon vertex detector installed in NOMAD, one of the neutrino oscillation experiments at the CERN-SPS. The use of the Kalman filter simplifies computationally the tracking and vertex procedure for NOMAD-STAR. The alignment of NOMAD-STAR is shown as an example of the application of the Kalman filter for tracking purposes. The accuracy of the method is such that one obtains alignment residuals between 9 and 12 μm . Furthermore, a preliminary measure of the impact parameter (with an RMS ∼36 μm ) illustrates the vertexing capabilities of thi…

PhysicsNuclear and High Energy PhysicsParticle physicsbusiness.industryPhysics::Instrumentation and DetectorsDetectorHigh Energy Physics::PhenomenologyFísicaKalman filterTracking (particle physics)Particle detectorSemiconductor detectorNeutrino detectorComputer visionFast Kalman filterHigh Energy Physics::ExperimentArtificial intelligenceDetectors and Experimental TechniquesNeutrino oscillationbusinessInstrumentation
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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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