Search results for "Oscillation"

showing 10 items of 1257 documents

Neutrino mixing and masses from long baseline and atmospheric oscillation experiments

1998

We argue that regardless of the outcome of future Long Baseline experiments, additional information will be needed to unambiguously decide among the different scenarios of neutrino mixing. We use, for this purpose, a simple test of underground data: an asymmetry between downward and upward going events. Such an asymmetry, in which matter effects can be crucial, tests electron and muon neutrino data separately and can be compared with the theoretical prediction without relying on any simulation program.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsOscillationmedia_common.quotation_subjectFísicaFOS: Physical sciencesElectronAsymmetryOutcome (probability)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentMuon neutrinoNeutrinoBaseline (configuration management)Mixing (physics)media_commonPhysics Letters B
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Advantages of locating LAGUNA in Pyhäsalmi mine

2011

Abstract LAGUNA is the next-generation underground Megaton-scale detector for the search for proton decay, for neutrino astrophysics and for the investigation of neutrino properties. A brief description of the three considered detector technologies is given and the main physics goals presented. While many of the research topics for LAGUNA are not affected by the geographical location of the detector, there are two areas where it is very important: low-energy neutrino measurements and long-baseline neutrino oscillations. Evaluation of the physics arguments in both cases indicates Pyhasalmi mine as the best European site for LAGUNA.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoDetectorGeophysicsSolar neutrino problemNeutrino detectorMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino astronomyNeutrinoNeutrino oscillationProgress in Particle and Nuclear Physics
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Neutrino oscillations refitted

2014

Here we update our previous global fit of neutrino oscillations by including the recent results which have appeared since the Neutrino-2012 conference. These include the measurements of reactor anti-neutrino disappearance reported by Daya Bay and RENO, together with latest T2K and MINOS data including both disappearance and appearance channels. We also include the revised results from the third solar phase of Super-Kamiokande, SK-III, as well as new solar results from the fourth phase of Super-Kamiokande, SK-IV. We find that the preferred global determination of the atmospheric angle $\theta_{23}$ is consistent with maximal mixing. We also determine the impact of the new data upon all the o…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoFOS: Physical sciencesFísicaSolar neutrino problemNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)MINOSMeasurements of neutrino speedHigh Energy Physics::ExperimentSensitivity (control systems)NeutrinoNeutrino oscillationMixing (physics)
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Testing neutrino mixing at future collider experiments

2000

Low energy supersymmetry with bilinear breaking of R-parity leads to a weak-scale seesaw mechanism for the atmospheric neutrino scale and a radiative mechanism for the solar neutrino scale. The model has striking implications for collider searches of supersymmetric particles. Assuming that the lightest SUSY particle is the lightest neutralino we demonstrate that (i) The neutralino decays inside the detector even for tiny neutrino masses. (ii) Measurements of the neutrino mixing angles lead to predictions for the ratios of various neutralino branching ratios implying an independent test of neutrino physics at future colliders, such as the Large Hadron Collider or a Linear Collider.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSolar neutrino problemLightest Supersymmetric Particlelaw.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Seesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)lawMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationColliderParticle Physics - Phenomenology
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A Supersymmetric Solution to the Solar and Atmospheric Neutrino Problems

1999

The simplest unified extension of the Minimal Supersymmetric Standard Model with bi-linear R--Parity violation provides a predictive scheme for neutrino masses which can account for the observed atmospheric and solar neutrino anomalies in terms of bi-maximal neutrino mixing. The maximality of the atmospheric mixing angle arises dynamically, by minimizing the scalar potential, while the solar neutrino problem can be accounted for either by large or by small mixing oscillations. One neutrino picks up mass by mixing with neutralinos, while the degeneracy and masslessness of the other two is lifted only by loop corrections. Despite the smallness of neutrino masses R-parity violation is observab…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSupersymmetrySolar neutrino problemHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)Minimal Supersymmetric Standard Model
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Combining first KamLAND results with solar neutrino data

2002

We consider the impact of the recent KamLAND data on neutrino oscillations, the first terrestrial neutrino experiment that can probe the solar neutrino anomaly. By combining the first 145.1 days of KamLAND data with the full sample of latest solar neutrino data we find an enhanced rejection against non-LMA oscillations, allowed only at more than 4 sigma with respect to LMA. Furthermore, the new data have a strong impact in narrowing down the allowed range of Delta_m^2 inside the LMA region. In contrast, our global analysis indicates that the new data have little impact on the location of the best fit point. In particular the solar neutrino mixing remains significantly non-maximal (3 sigma).

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoSigmaFOS: Physical sciencesFísicaSolar neutrino problemHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedHigh Energy Physics::ExperimentAnomaly (physics)NeutrinoNeutrino oscillationMixing (physics)
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Direct neutrino mass measurements

1995

The paper reports on recent progress and developments since the neutrino '92 conference in the search for finite neutrino masses by direct mass measurements. Regarding the mass of μ - and τ -neutrino experiments have been finished and come up with somewhat improved upper bounds; the negative m 2 -value for the μ -neutrino could be removed mostly. Indications of a 17 keV neutrino component in β -decay spectra have been disproved by a number of alternative experiments as well as by reanalysis of part of the original data. Regarding the electron neutrino mass, measurements by magnetic spectrometers are phasing out in favour of electrostatic filters with magnetic guiding fields. These experimen…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoSolar neutrino problemAtomic and Molecular Physics and OpticsMuon captureNuclear physicsNeutrino detectorMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationElectron neutrinoNuclear Physics B - Proceedings Supplements
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The strong CP problem and the solar neutrino puzzle: Are they related?

1991

We discuss the possibility that a solution of the strong CP problem via the introduction of a chiral U(1), a la Peccei-Quinn, may also provide a natural scenario for explaining the apparent depletion of the solar neutrino flux through matter enhanced neutrino oscillations. The smallness of the neutrino masses is related to the scale at which the U(1)PQ symmetry is spontaneously broken, without introducing right-handed neutrino fields and invoking the see-saw mechanism. The model is consistent with all present experimental results. In particular, the phenomenology associated to the presence of an “invisible” axion is the same as in the Dine-Fischler-Srednicki-Zhitnisky model with the excepti…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSpontaneous symmetry breakingSolar neutrinoHigh Energy Physics::PhenomenologyElementary particleStrong CP problemNeutrinoNeutrino oscillationPhenomenology (particle physics)AxionNuclear Physics B
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Vector current conservation and neutrino emission from singlet-paired baryons in neutron stars

2006

Neutrino emission caused by singlet Cooper pairing of baryons in neutron stars is recalculated by accurately taking into account for conservation of the vector weak currents. The neutrino emissivity via the vector weak currents is found to be several orders of magnitude smaller than that obtained before by different authors. This makes unimportant the neutrino radiation from singlet pairing of protons or hyperons.

PhysicsNuclear and High Energy PhysicsParticle physicsProtonAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)Nuclear TheoryHigh Energy Physics::PhenomenologyHyperonFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsPartícules (Física nuclear)BaryonNuclear physicsHigh Energy Physics - PhenomenologyNeutron starHigh Energy Physics - Phenomenology (hep-ph)PairingHigh Energy Physics::ExperimentNeutrinoCooper pairNeutrino oscillationNuclear ExperimentPhysics Letters B
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A precise measurement of the muon neutrino nucleon inclusive charged current cross section off an isoscalar target in the energy range 2.5

2008

Abstract We present a measurement of the muon neutrino–nucleon inclusive charged current cross section, off an isoscalar target, in the neutrino energy range 2.5 ⩽ E ν ⩽ 40 GeV . The significance of this measurement is its precision, ±4% in 2.5 ⩽ E ν ⩽ 10 GeV , and ±2.6% in 10 ⩽ E ν ⩽ 40 GeV regions, where significant uncertainties in previous experiments still exist, and its importance to the current and proposed long baseline neutrino oscillation experiments.

PhysicsNuclear and High Energy PhysicsParticle physicsRange (particle radiation)Muon010308 nuclear & particles physicsIsoscalarAstrophysics::High Energy Astrophysical Phenomena01 natural sciencesNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Muon neutrinoHigh Energy Physics::ExperimentNeutrino010306 general physicsNucleonNeutrino oscillationNuclear ExperimentCharged current
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