Search results for "neutrino oscillation"

showing 10 items of 521 documents

Neutrino phenomenology and stable dark matter with A4

2011

We present a model based on the A4 non-abelian discrete symmetry leading to a predictive five-parameter neutrino mass matrix and providing a stable dark matter candidate. We found an interesting correlation among the atmospheric and the reactor angles which predicts theta_23 ~ pi/4 for very small reactor angle and deviation from maximal atmospheric mixing for large theta_13. Only normal neutrino mass spectrum is possible and the effective mass entering the neutrinoless double beta decay rate is constrained to be |m_ee| > 4 10^{-4} eV.

Nuclear and High Energy PhysicsParticle physicsLepton mixingDark matterDiscrete symmetriesFOS: Physical sciencesElementary particle01 natural sciences7. Clean energyNuclear physicsEffective mass (solid-state physics)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesDark matterNeutrinoless double beta decay010306 general physicsNeutrino oscillationPhysics010308 nuclear & particles physicsFlavor symmetriesNeutrino massesMassless particleHigh Energy Physics - PhenomenologyMass spectrumNeutrinoPhysics Letters B
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What can we learn from neutrinoless double beta decay experiments?

2004

We assess how well next generation neutrinoless double beta decay and normal neutrino beta decay experiments can answer four fundamental questions. 1) If neutrinoless double beta decay searches do not detect a signal, and if the spectrum is known to be inverted hierarchy, can we conclude that neutrinos are Dirac particles? 2) If neutrinoless double beta decay searches are negative and a next generation ordinary beta decay experiment detects the neutrino mass scale, can we conclude that neutrinos are Dirac particles? 3) If neutrinoless double beta decay is observed with a large neutrino mass element, what is the total mass in neutrinos? 4) If neutrinoless double beta decay is observed but ne…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryFOS: Physical sciencesAstrophysics01 natural sciencesNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesMass scaleNuclear Experiment (nucl-ex)010306 general physicsNeutrino oscillationNuclear ExperimentPhysicsMass element010308 nuclear & particles physicsDirac (video compression format)Astrophysics (astro-ph)High Energy Physics::PhenomenologyBeta decayHigh Energy Physics - PhenomenologyAstronomiaHigh Energy Physics::ExperimentNeutrinoMass hierarchy
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Neutrino-nucleus quasi-elastic and 2p2h interactions up to 10 GeV

2013

We extend to 10 GeV results from a microscopic calculation of charged-current neutrino-nucleus reactions that do not produce a pion in the final state. For the class of events coming from neutrino interactions with two nucleons producing two holes (2p2h), limiting the calculation to three-momentum transfers less than 1.2 GeV produces a two-dimensional distribution in momentum and energy transfer that is roughly constant as a function of energy. The cross section for 2p2h interactions approximately scales with the number of nucleons for isoscalar nuclei, similar to the quasi-elastic cross section. When limited to momentum transfers below 1.2 GeV, the cross section is 26% of the quasi-elastic…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryIsoscalarFOS: Physical sciences01 natural sciences7. Clean energyScatteringNuclear Theory (nucl-th)Nuclear physicsMomentumCross section (physics)High Energy Physics - Phenomenology (hep-ph)Pion0103 physical sciencesNuclear Experiment010306 general physicsNeutrino oscillationPhysicsMeson-exchange currents010308 nuclear & particles physicsMomentum transferHigh Energy Physics - PhenomenologyFísica nuclearHigh Energy Physics::ExperimentNeutrinoNucleonPhysical Review D
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A road map to solar neutrino fluxes, neutrino oscillation parameters, and tests for new physics

2003

We analyze all available solar and related reactor neutrino experiments, as well as simulated future 7Be, p-p, pep, and ^8B solar neutrino experiments. We treat all solar neutrino fluxes as free parameters subject to the condition that the total luminosity represented by the neutrinos equals the observed solar luminosity (the `luminosity constraint'). Existing experiments show that the p-p solar neutrino flux is 1.02 +- 0.02 (1 sigma) times the flux predicted by the BP00 standard solar model; the 7Be neutrino flux is 0.93^{+0.25}_{-0.63} the predicted flux; and the ^8B flux is 1.01 +- 0.04 the predicted flux. The neutrino oscillation parameters are: Delta m^2 = 7.3^{+0.4}_{-0.6}\times 10^{-…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryPhysics beyond the Standard ModelSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaSolar luminosityFOS: Physical sciencesAstrophysics7. Clean energy01 natural sciencesLuminosityHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear fusionAstrophysics::Solar and Stellar AstrophysicsNuclear Experiment (nucl-ex)010306 general physicsNeutrino oscillationNuclear ExperimentParticle Physics - PhenomenologyPhysicsStandard solar model010308 nuclear & particles physicsAstrophysics (astro-ph)FísicaHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsNeutrino
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Solar Neutrinos Before and After Neutrino 2004

2004

We compare, using a three neutrino analysis, the allowed neutrino oscillation parameters and solar neutrino fluxes determined by the experimental data available Before and After Neutrino 2004. New data available after Neutrino2004 include refined KamLAND and gallium measurements. We use six different approaches to analyzing the KamLAND data. We present detailed results using all the available neutrino and anti-neutrino data for Delta m^2_{12}, tan^2 theta_{12}, sin^2 theta_{13}, and sin^2 eta (sterile fraction). Using the same complete data sets, we also present Before and After determinations of all the solar neutrino fluxes, which are treated as free parameters, an upper limit to the lumi…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryPhysics::Instrumentation and DetectorsSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesAstrophysics01 natural sciences7. Clean energyLuminosityNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNeutrino oscillationNuclear ExperimentPhysicsStandard solar model010308 nuclear & particles physicsScatteringOscillationAstrophysics (astro-ph)High Energy Physics::PhenomenologyFísicaSigmaHigh Energy Physics - Phenomenology13. Climate actionHigh Energy Physics::ExperimentNeutrino
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Robust signatures of solar neutrino oscillation solutions

2001

With the goal of identifying signatures that select specific neutrino oscillation parameters, we test the robustness of global oscillation solutions that fit all the available solar and reactor experimental data. We use three global analysis strategies previously applied by different authors and also determine the sensitivity of the oscillation solutions to the critical nuclear fusion cross section, S_{17}(0), for the production of 8B. The favored solutions are LMA, LOW, and VAC in order of g.o.f. The neutral current to charged current ratio for SNO is predicted to be 3.5 +- 0.6 (1 sigma), which is separated from the no-oscillation value of 1.0 by much more than the expected experimental er…

Nuclear and High Energy PhysicsParticle physicsNuclear TheorySolar neutrinoFOS: Physical sciencesAstrophysics01 natural sciences7. Clean energyHigh Energy Physics - ExperimentStandard ModelNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNeutrino oscillationNuclear ExperimentBorexinoCharged currentParticle Physics - PhenomenologyPhysicsStandard solar model010308 nuclear & particles physicsOscillationAstrophysics (astro-ph)FísicaHigh Energy Physics - Phenomenology13. Climate actionHigh Energy Physics::ExperimentNeutrino
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Photon emission in neutral-current interactions at intermediate energies

2013

Neutral current photon emission reactions with nucleons and nuclei are studied. These processes are important backgrounds for nu_mu to nu_e (bar(nu)_mu to bar(nu)_e) appearance oscillation experiments where electromagnetic showers instigated by electrons (positrons) and photons are not distinguishable. At intermediate energies, these reactions are dominated by the weak excitation of the Delta(1232) resonance and its subsequent decay into Ngamma There are also non-resonant contributions that, close to threshold, are fully determined by the effective chiral Lagrangian of strong interactions. In addition, we have also included mechanisms mediated by nucleon excitations (N*) from the second res…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryStrong interactionNuclear TheoryFOS: Physical sciencesElectron01 natural sciencesResonance (particle physics)High Energy Physics - ExperimentNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Experiment (hep-ex)Pauli exclusion principleHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationNuclear ExperimentPhysicsNeutral current010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics - Phenomenology13. Climate actionsymbolsHigh Energy Physics::ExperimentNeutrinoAtomic physicsNucleon
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Atmospheric neutrino oscillations and new physics

2004

We study the robustness of the determination of the neutrino masses and mixing from the analysis of atmospheric and K2K data under the presence of different forms of phenomenologically allowed new physics in the nu_mu--nu_tau sector. We focus on vector and tensor-like new physics interactions which allow us to treat, in a model independent way, effects due to the violation of the equivalence principle, violations of the Lorentz invariance both CPT conserving and CPT violating, non-universal couplings to a torsion field and non-standard neutrino interactions with matter. We perform a global analysis of the full atmospheric data from SKI together with long baseline K2K data in the presence of…

Nuclear and High Energy PhysicsParticle physicsOscillationsPhysics beyond the Standard ModelFOS: Physical sciencesLorentz covariance01 natural sciencesTorsion fieldPartícules (Física nuclear)High Energy Physics - Phenomenology (hep-ph)Robustness (computer science)0103 physical sciencesOscil·lacionsNeutrinsNeutrinos010306 general physicsNeutrino oscillationMixing (physics)Particles (Nuclear physics)PhysicsViolació càrrega-paritat (Física nuclear)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoAtmospheric neutrinoCP violation (Nuclear physics)Physical Review D
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Determination of the atmospheric neutrino flux and searches for new physics with AMANDA-II

2009

The AMANDA-II detector, operating since 2000 in the deep ice at the geographic South Pole, has accumulated a large sample of atmospheric muon neutrinos in the 100 GeV to 10 TeV energy range. The zenith angle and energy distribution of these events can be used to search for various phenomenological signatures of quantum gravity in the neutrino sector, such as violation of Lorentz invariance (VLI) or quantum decoherence (QD). Analyzing a set of 5511 candidate neutrino events collected during 1387 days of livetime from 2000 to 2006, we find no evidence for such effects and set upper limits on VLI and QD parameters using a maximum likelihood method. Given the absence of evidence for new flavor-…

Nuclear and High Energy PhysicsParticle physicsOscillationsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaConfidence-IntervalsGravityFOS: Physical sciencesGeneratorLorentz covariance01 natural sciences7. Clean energyHigh Energy Physics - ExperimentScatteringHigh Energy Physics - Experiment (hep-ex)SensitivityQuantum Decoherence0103 physical sciencesddc:530Muon neutrino010306 general physicsNeutrino oscillationTelescopeAstroparticle physicsPhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySolar neutrino problemNeutrino detector13. Climate actionMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoAstrophysics - High Energy Astrophysical PhenomenaSmall SignalsLorentz Invariance Violation
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Gravitino dark matter and neutrino masses with bilinear R-parity violation

2011

Bilinear R-parity violation provides an attractive origin for neutrino masses and mixings. In such schemes the gravitino is a viable decaying dark matter particle whose R-parity violating decays lead to monochromatic photons with rates accessible to astrophysical observations. We determine the parameter region allowed by gamma-ray line searches, dark matter relic abundance and neutrino oscillation data, obtaining a limit on the gravitino mass $m_{\tilde G} \lsim$ 1-10 GeV corresponding to a relatively low reheat temperature $T_R \lsim$ few $\times 10^7-10^8$ GeV. Neutrino mass and mixing parameters may be reconstructed at accelerator experiments like the Large Hadron Collider.

Nuclear and High Energy PhysicsParticle physicsPhotonAstrophysics::High Energy Astrophysical PhenomenaDark matterFOS: Physical sciencesMasas de neutrinos01 natural sciencesNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)R-paridad bilinealR-parity0103 physical sciences010306 general physicsNeutrino oscillationLine (formation)PhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyGravitinoHigh Energy Physics::ExperimentNeutrinoGravitino
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