Search results for "neutrino oscillation"

showing 10 items of 521 documents

Physics potential of the Jiangmen underground neutrino observatory

2019

JUNO (Jiangmen Underground Neutrino Observatory) is a 20 kton multipurpose neutrinodetector under construction in China and it will be completed in 2021. The detector will belocated near the the city of Jiangmen, 53 km away from two nuclear power plants that willprovide the neutrino flux for the main sear of the observatory. The main physics goal is the determination of the neutrino Mass Hierarchy, even if will play animportant also in other topics, such as: neutrino oscillation, solar neutrino, SuperNova neutrinos,geoneutrinos and atmosperic neutrinos among others

PhysicsPhysics::Instrumentation and Detectorsbusiness.industryAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyAstronomyFluxNuclear powerneutrinoSupernovaObservatoryHigh Energy Physics::ExperimentNeutrinobusinessNeutrino oscillationJiangmen Underground Neutrino Observatory
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Limits on diffuse fluxes of high energy extraterrestrial neutrinos with the AMANDA-B10 detector

2003

Data from the AMANDA-B10 detector taken during the austral winter of 1997 have been searched for a diffuse flux of high energy extraterrestrial muon-neutrinos, as predicted from, e.g., the sum of all active galaxies in the universe. This search yielded no excess events above those expected from the background atmospheric neutrinos, leading to upper limits on the extraterrestrial neutrino flux. For an assumed E^-2 spectrum, a 90% classical confidence level upper limit has been placed at a level E^2 Phi(E) = 8.4 x 10^-7 GeV cm^-2 s^-1 sr^-1 (for a predominant neutrino energy range 6-1000 TeV) which is the most restrictive bound placed by any neutrino detector. When specific predicted spectral…

PhysicsPhysics::Instrumentation and Detectorsmedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyQuasarCosmic rayAstrophysicsAstrophysicsUniverseMassless particlePhysics::Popular PhysicsExtraterrestrial lifeHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLeptonmedia_common
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The beta-, neutrino- and proton-asymmetry in neutron beta-decay

2004

This article describes measurements of angular-correlation coefficients in the decay of free neutrons with the superconducting spectrometer PERKEO II. A method for measuring the β-asymmetry coefficient A is presented, as well as a new method for determining the neutrino-asymmetry coefficient B, which allows a value for the proton-asymmetry coefficient C to be obtained for the first time. An ongoing experiment is trying to improve the accuracy of these quantities.

PhysicsProtonSolar neutrinomedia_common.quotation_subjectneutron β-decayGeneral Engineeringangular-correlation coefficientsAsymmetryArticleNuclear physicsBeta (plasma physics)High Energy Physics::ExperimentSuperconducting spectrometerNeutronNeutrinoNeutrino oscillationmedia_commonJournal of Research of the National Institute of Standards and Technology
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Features of quark and lepton mixing from differential geometry of curves on surfaces

1998

It is noted that the CKM matrix elements for both quarks and leptons as conceived in the Dualized Standard Model (DSM) can be interpreted as direction cosines obtained by moving the Darboux trihedron (a 3-frame) along a trajectory on a sphere traced out through changing energy scales by a 3-vector factorized from the mass matrix. From the `Darboux' analogues of the well-known Serret--Frenet formulae for space curves, it is seen that the corner elements ($V_{ub}, V_{td}$ for quarks, and $U_{e3}, U_{\tau 1}$ for leptons) are associated with the (geodesic) torsion, while the other off-diagonal elements ($V_{us}, V_{cd}$ and $V_{cb}, V_{ts}$ for quarks, and $U_{e2}, U_{\mu 1}$ and $U_{\mu 3}, U…

PhysicsQuarkHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsGeodesicCabibbo–Kobayashi–Maskawa matrixHadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaMass matrixMatrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)High Energy Physics::ExperimentNeutrino oscillationLepton
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Relating quarks and leptons without grand-unification

2011

In combination with supersymmetry, flavor symmetry may relate quarks with leptons, even in the absence of a grand-unification group. We propose an SU(3)xSU(2)xU(1) model where both supersymmetry and the assumed A4 flavor symmetries are softly broken, reproducing well the observed fermion mass hierarchies and predicting: (i) a relation between down-type quarks and charged lepton masses, and (ii) a correlation between the Cabibbo angle in the quark sector, and the reactor angle characterizing CP violation in neutrino oscillations.

PhysicsQuarkNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSupersymmetry01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesCP violationGrand Unified TheoryHigh Energy Physics::Experiment010306 general physicsNeutrino oscillationLepton
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A dynamical mechanism for quark mixing and neutrino oscillations

1999

We show that assuming fermion generations to be given by a gauge symmetry plus a certain Higgs mechanism for its breaking, the known empirical features of quark and lepton mixing can be largely explained, including in particular the fact that the mixing (CKM) matrix element $U_{\mu3}$ responsible for the muon anomaly in atmospheric neutrinos is near maximal and much larger than their quark counterparts $V_{cb}$ and $ V_{ts}$, while the corner elements for both quarks ($V_{ub}, V_{td}$) and leptons ($U_{e3}$) are all very small. The mechanism also gives automatically a hierarchical fermion mass spectrum which is intimately related to the mixing pattern.

PhysicsQuarkParticle physicsMuonPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesFermionHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)symbolsHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationEngineering (miscellaneous)Higgs mechanismMixing (physics)LeptonThe European Physical Journal C
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Quark and lepton mixing in weak interactions

1986

The coupling strength of weak interactions between quarks of different flavour shows a clear pattern: couplings between members of the same family are much stronger than the ones between neighbour families and couplings between first and third family haye escaped detection so far. The coupling strength between different families decreases with increasing quark mass, but a theoretical explanation of this pattern is still missing. On the other side, lepton mixing and neutrino oscillations have not been seen in experiments yet. An analysis of experimental data in the framework of simultaneous oscillations of three neutrino fluxes yields limits on the three mixing angles which are about as rest…

PhysicsQuarkTop quarkParticle physicsHigh Energy Physics::PhenomenologyUp quarkDown quarkHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationBottom quarkLepton
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A calorimeter for the precise determination of the activity of the 144Ce-144Pr anti-neutrino source in the SOX experiment

2018

We describe the design and the performance of a high precision thermal calorimeter, whose purpose was the measurement of the total activity of the 144Ce-144Pr anti-neutrino source of the SOX (Short distance neutrino Oscillation with BoreXino) experiment. SOX aimed at the search for eV-scale sterile neutrinos by means of the Borexino detector at the Laboratori Nazionali del Gran Sasso in Italy and of a very powerful artificial anti-neutrino source located at 8.51 m from the detector center. In order to obtain the required sensitivity, the activity of the source (approximately 150 kCi) had to be known at 1% precision. In this work we report the design of the experimental apparatus and the res…

PhysicsRadiation monitoringPhysics::Instrumentation and Detectors010308 nuclear & particles physicsDetector01 natural sciencesParticle detectorCalorimeterNuclear physicsCalorimetersNeutrino detectorMockup0103 physical sciencesHigh Energy Physics::ExperimentNeutrinoCalorimeters; Radiation monitoring; Instrumentation; Mathematical Physics010306 general physicsNeutrino oscillationInstrumentationMathematical PhysicsBorexinoJournal of Instrumentation
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Neutrino flux prediction at MiniBooNE

2009

The booster neutrino experiment (MiniBooNE) searches for nu(mu)->nu(e) oscillations using the O(1 GeV) neutrino beam produced by the booster synchrotron at the Fermi National Accelerator Laboratory). The booster delivers protons with 8 GeV kinetic energy (8.89 GeV/c momentum) to a beryllium target, producing neutrinos from the decay of secondary particles in the beam line. We describe the Monte Carlo simulation methods used to estimate the flux of neutrinos from the beam line incident on the MiniBooNE detector for both polarities of the focusing horn. The simulation uses the Geant4 framework for propagating particles, accounting for electromagnetic processes and hadronic interactions in the…

PhysicsResearch Groups and Centres\Physics\Low Temperature PhysicsNuclear and High Energy PhysicsParticle physicsMesonFaculty of Science\PhysicsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesHigh Energy Physics - ExperimentMassless particleMiniBooNENuclear physicsHigh Energy Physics - Experiment (hep-ex)PionPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilabNeutrinoNuclear ExperimentNeutrino oscillationLeptonPhysical Review D
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Expected performance of an ideal liquid argon neutrino detector with enhanced sensitivity to scintillation light

2014

Scintillation light is used in liquid argon (LAr) neutrino detectors to provide a trigger signal, veto information against cosmic rays, and absolute event timing. In this work, we discuss additional opportunities offered by detectors with enhanced sensitivity to scintillation light, that is with light collection efficiencies of about $10^{-3}$. We focus on two key detector performance indicators for neutrino oscillation physics: calorimetric neutrino energy reconstruction and neutrino/antineutrino separation in a non-magnetized detector. Our results are based on detailed simulations, with neutrino interactions modelled according to the GENIE event generator, while the charge and light respo…

PhysicsScintillationPhysics - Instrumentation and DetectorsMuonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)7. Clean energyHigh Energy Physics - ExperimentMuon captureNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Neutrino detectorHigh Energy Physics::ExperimentMuon neutrinoNeutrinoNeutrino oscillationInstrumentationElectron neutrinoMathematical PhysicsJournal of Instrumentation
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