Search results for "oscillation"

showing 10 items of 1257 documents

Neutrino mass and new light gauge boson in superstring models

1987

Abstract The proposal that the neutrino owes the smallness of its mass to the spontaneous breaking of R parity in superstring models with an additional gauge boson coupled to the right-handed neutrino is analysed. The right-handed neutrino can not in general decouple from the low-energy theory in models with supersymmetry at the TeV scale and which possess the light Higgs doublets necessary for generating fermion masses. Experimental limits on neutrino mass then imply an upper limit on the new gauge boson mass m Zr ⪅ 220 GeV.

PhysicsNuclear and High Energy PhysicsGauge bosonSterile neutrinoParticle physicsNeutrino theory of lightAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologySupersymmetryHigh Energy Physics::TheoryHiggs bosonMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationPhysics Letters B
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Simpson's neutrino and the singular seesaw

1991

We derive explicit forms for the neutrino and lepton "mixing-matrices" which describe the generic singular see-saw model. The dependence on the hierarchy parameter is contrasted with the non-singular case. Application is made to Simpson's 17 keV neutrino.

PhysicsNuclear and High Energy PhysicsHierarchyParticle physicsParticle modelPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFísicaAstronomy and AstrophysicsElementary particleFermionMassless particleHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLepton
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Optimal β-beam at the CERN-SPS

2005

A β-beam with maximum (for 6He ions) or (for 18Ne) could be achieved at the CERN-SPS. We study the sensitivity to and δ of such a beam as function of γ, optimizing with the baseline constrained to CERN–Frejus (130 km), and also with simultaneous variation of the baseline, for a fixed ion flux. These results are compared to the standard scenario previously considered, with lower , and also with a higher option that requires a more powerful accelerator. We conclude that the sensitivity to CP violation and increases significantly with γ if the baseline is increased proportionally, while for the CERN–Frejus scenario the dependence on γ is mild provided γ is above 100.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderIon beamAstrophysics::High Energy Astrophysical PhenomenaAnalytical chemistryFluxIonNuclear physicsHigh Energy Physics - PhenomenologyPhysics::Accelerator PhysicsCP violationNeutrino oscillationBeam (structure)Charged currentParticle Physics - PhenomenologyNuclear Physics B
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A $B_4C$-silicon target for the detection of neutrino interactions

1998

This note describes the construction of a target for neutrino interactions composed of passive boron carbide plates interleaved with silicon microstrip detectors. The target contains four layers of passive material with a total mass of 45 kg and 600 single--sided silicon microstrip detectors with a total surface of 1.14 m$^2$ distributed over five layers. It is installed in the NOMAD spectrometer at the CERN SPS neutrino beam. During the 1997 run about 8000 \nm\ charged current interactions were estimated to have occurred in the target. For these events it will be possible to perform a precise measurement of both vertex and kinematical variables. This will provide invaluable experience towa…

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderSpectrometerSiliconPhysics::Instrumentation and DetectorsFísicachemistry.chemical_elementsilicon microstrip detectors; neutrino oscillations; silicon strip sensors; tracking detectors; search; alignmentNuclear physicsNeutrino detectorchemistryMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationInstrumentationCharged currentParticle Physics - Experiment
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Inclusive muon capture in light nuclei

1998

We study total muon capture rates in light nuclei, taking into account renormalizations of the nuclear vector and axial vector strengths. We estimate the influence in the results of uncertainties of the spin-isospin interaction parameter and nuclear densities. A few of these reactions are theoretical benchmarks for physics involving searches for neutrino oscillations. New experiments in muon capture in several targets are suggested, in the light of some discrepancies with theory, crudeness of some experimental results and relevance to neutrino physics.

PhysicsNuclear and High Energy PhysicsLight nucleusNuclear TheoryPhysics::Instrumentation and DetectorsNuclear TheoryFOS: Physical sciencesFísicaMuon captureNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics::ExperimentNeutrinoNuclear ExperimentStudy.totalNeutrino oscillationPseudovectorPhysics Letters B
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RECENT RESULTS FROM AMANDA

2001

We present results based on data taken in 1997 with the 302-PMT Antarctic Muon and Neutrino Detector Array-B10 ("AMANDA-B10") array. Atmospheric neutrinos created in the northern hemisphere are observed indirectly through their charged current interactions which produce relativistic, Cherenkov-light-emitting upgoing muons in the South Pole ice cap. The reconstructed angular distribution of these events is in good agreement with expectation and demonstrates the viability of this ice-based device as a neutrino telescope.

PhysicsNuclear and High Energy PhysicsMuonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoAstrophysics::Instrumentation and Methods for AstrophysicsAstronomyAstronomy and AstrophysicsAstrophysicsSolar neutrino problemAtomic and Molecular Physics and OpticsNeutrino detectorMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationPhysics::Atmospheric and Oceanic PhysicsCharged currentInternational Journal of Modern Physics A
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Derivation of transient relativistic fluid dynamics from the Boltzmann equation for a multi-component system

2012

We derive the non-equilibrium single-particle momentum distribution function of a hadron resonance gas. We then study the effects that this newly derived expression can have in the freeze-out description of fluid-dynamical models of heavy ion collisions and compare it with the method traditionally employed, the 14-moment approximation.

PhysicsNuclear and High Energy PhysicsNuclear Theoryta114Component (thermodynamics)Dynamics (mechanics)HadronFOS: Physical sciencesBoltzmann equationResonance (particle physics)MomentumNuclear Theory (nucl-th)High Energy Physics - PhenomenologyClassical mechanicsDistribution functionHigh Energy Physics - Phenomenology (hep-ph)Statistical physicsTransient (oscillation)Nuclear ExperimentNuclear Physics A
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Density and geometry of single component plasmas

2007

Abstract The density and geometry of p ¯ and e + plasmas in realistic trapping potentials are required to understand and optimize antihydrogen ( H ¯ ) formation. An aperture method and a quadrupole oscillation frequency method for characterizing such plasmas are compared for the first time, using electrons in a cylindrical Penning trap. Both methods are used in a way that makes it unnecessary to assume that the plasmas are spheroidal, and it is shown that they are not. Good agreement between the two methods illustrates the possibility to accurately determine plasma densities and geometries within non-idealized, realistic trapping potentials.

PhysicsNuclear and High Energy PhysicsOscillationGeometryPlasmaTrappingElectronPenning trapPhysics::Plasma PhysicsUpper hybrid oscillationQuadrupolePhysics::Atomic PhysicsAtomic physicsDetectors and Experimental TechniquesAntihydrogen
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Prospects for the Zee-Babu Model at the LHC and low energy experiments

2007

We analyze the viability of the Zee-Babu model as an explanation of observed neutrino masses and mixings and the possibility that the model is confirmed or discarded in experiments planned for the very close future. The allowed parameter space is studied analytically by using some approximations and partial data. Then, a complete scanning of all parameters and constraints is performed numerically by using Monte Carlo methods. The cleanest signal of the model will be the detection of the doubly charged scalar at the LHC and its correlation with measurements of the branching ratio of $\mu\to e\gamma$ at the MEG experiment. In addition, the model offers interesting predictions for $\tau^{-}\to…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionHadronMonte Carlo methodHigh Energy Physics::PhenomenologyDrell–Yan processFOS: Physical sciencesParameter space7. Clean energy01 natural sciencesPartícules (Física nuclear)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillation
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Probing new physics by comparing solar and KamLAND data

2004

We explore whether KamLAND and solar data may end up inconsistent when analyzed in terms of two-flavor neutrino oscillations. If this turned out to be the case, one would be led to conclude that there is more new physics, besides neutrino masses and mixing, in the leptonic sector. On the other hand, given that KamLAND and solar data currently agree when analyzed in terms of two-flavor neutrino oscillations, one is able to place nontrivial bounds on several manifestations of new physics. In particular, we compute how well a combined KamLAND and solar data analysis is able to constrain a specific form of violation of CPT invariance by placing a very stringent upper bound, |Delta m^2 - Delta b…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCPT symmetryPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaWeinberg angleParameter space01 natural sciencesUpper and lower boundsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesInvariant massHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillation
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