Search results for "Measurements"

showing 10 items of 720 documents

Relic Neutrino Decoupling Including Flavour Oscillations

2005

In the early universe, neutrinos are slightly coupled when electron-positron pairs annihilate transferring their entropy to photons. This process originates non-thermal distortions on the neutrino spectra which depend on neutrino flavour, larger for nu_e than for nu_mu or nu_tau. We study the effect of three-neutrino flavour oscillations on the process of neutrino decoupling by solving the momentum-dependent kinetic equations for the neutrino spectra. We find that oscillations do not essentially modify the total change in the neutrino energy density, giving N_eff=3.046 in terms of the effective number of neutrinos, while the small effect over the production of primordial 4He is increased by…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFlavourAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaNeutrino decouplingSolar neutrino problemAstrophysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLepton
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Solar neutrinos as probes of neutrino–matter interactions

2004

Data from solar neutrino and KamLAND experiments have led to a discovery of nonzero neutrino masses. Here we investigate what these data can tell us about neutrino interactions with matter, including the poorly constrained flavor-changing nu_e-nu_tau interactions. We give examples of the interaction parameters that are excluded by the solar/KamLAND data and are beyond the reach of other experiments. We also demonstrate that flavor-changing interactions, at the allowed level, may profoundly modify the conversion probability for neutrinos of energy <~ 6 MeV and the values of the mass parameter inferred from the data. The implications for future experiments are discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsSolar neutrinoHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaElementary particleSolar neutrino problem01 natural sciences7. Clean energyNuclear physicsMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)13. Climate action0103 physical sciencesMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationLeptonPhysics Letters B
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Working group on neutrino physics and astrophysics — concluding remarks I

1998

Abstract This part of the concluding remarks on the contributions and discussions in the working group on Neutrino Physics and Astrophysics summarises the following items: 1. 1) Neutrino mass measurement from Tritium beta decay, 2. 2) Neutrinoless double beta decay, 3. 3) Application of cryodetectors to the determination of neutrino properties, 4. 4) Search for a magnetic moment of the neutrino and, 5. 5) Limits on the mass of the Tau neutrino

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoHigh Energy Physics::PhenomenologyAstrophysicsSolar neutrino problemAtomic and Molecular Physics and OpticsNuclear physicsTau neutrinoDouble beta decayMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLeptonNuclear Physics B - Proceedings Supplements
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Fitting Simpson's neutrino into the standard model

1985

Abstract I show how to accomodate the 17 keV state recently reported by Simpson as one of the neutrinos of the standard model. Experimental constraints can only be satisfied if the μ and τ neutrino combine to a very good approximation to form a Dirac neutrino of 17 keV leaving a light ν e . Neutrino oscillations will provide the most stringent test of the model. The cosmological bounds are also satisfied in a natural way in models with Goldstone bosons. Explicit examples are given in the framework of majoron-type models. Constraints on the lepton symmetry breaking scale which follow from astrophysics, cosmology and laboratory experiments are discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsDirac (video compression format)Astrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFísicaStandard ModelGoldstone bosonMeasurements of neutrino speedHigh Energy Physics::ExperimentSymmetry breakingNeutrinoNeutrino oscillationParticle Physics - PhenomenologyLepton
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The KATRIN sensitivity to the neutrino mass and to right-handed currents in beta decay

2007

The aim of the KArlsruhe TRItium Neutrino experiment KATRIN is the determination of the absolute neutrino mass scale down to 0.2 eV, with essentially smaller model dependence than from cosmology and neutrinoless double beta decay. For this purpose, the integral electron energy spectrum is measured close to the endpoint of molecular tritium beta decay. The endpoint, together with the neutrino mass, should be fitted from the KATRIN data as a free parameter. The right-handed couplings change the electron energy spectrum close to the endpoint, therefore they have some effect also to the precise neutrino mass determination. The statistical calculations show that, using the endpoint as a free par…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsFOS: Physical sciencesBeta decayCosmologyNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationFree parameterKATRIN
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Subleading effects in the 1-2 sector: Non-standard neutrino interactions

2005

We have reconsidered the status of the large mixing angle (LMA) oscillation (OSC) interpretation of the solar neutrino data in a more general framework where non-standard neutrino interactions (NSI) are present. Using the latest data from all solar neutrino experiments and KamLAND we have found the existence of three LMA solutions, instead of the unique solution which holds in the absence of NSI, LMA-I. In addition to LMA-I, there is another solution with smaller Δ m 2 (LMA-0), and a new “dark-side” solution (LMA-D) with sin 2 θ = 0.70 . We comment on the potential of KamLAND and future solar neutrino experiments using 7Be and 8B neutrinos to lift the degeneracy between the LMA-I, LMA-0 and…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsOscillationSolar neutrinoSolar neutrino problemAtomic and Molecular Physics and OpticsMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoDegeneracy (mathematics)Neutrino oscillationMixing (physics)Nuclear Physics B - Proceedings Supplements
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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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