Search results for " Neutrino"

showing 10 items of 727 documents

Update analysis of : Theory and Experiment

2009

Within the resonance chiral theory (RχT), we have studied the process of a tau lepton decaying into a vector resonance plus a pseudo-Goldstone meson and a tau neutrino. Two kinds of processes are discussed: (a) τ − → ( ρ 0 π − , ω π − , ϕ π − , K ∗ 0 K − ) ν τ , belonging to Δ S = 0 processes and (b) Δ S = 1 processes, such as τ − → ( ρ 0 K − , ω K − , ϕ K − , K ¯ ∗ 0 π − ) ν τ . To fit the τ − → ω π − ν τ spectral function and the decay distribution of τ − → ω K − ν τ to get unknown resonance couplings, we then make a prediction for branching ratios of all channels.

PhysicsNuclear and High Energy PhysicsParticle decayPionBranching fractionTau neutrinoResonanceAtomic physicsOmega baryonAtomic and Molecular Physics and OpticsLeptonDimensionless quantityNuclear Physics B - Proceedings Supplements
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A combined beta-beam and electron capture neutrino experiment

2009

The next generation of long baseline neutrino experiments will aim at determining the value of the unknown mixing angle, theta_{13}, the type of neutrino mass hierarchy and the presence of CP-violation in the lepton sector. Beta-beams and electron capture experiments have been studied as viable candidates for long baseline experiments. They use a very clean electron neutrino beam from the beta-decays or electron capture decays of boosted ions. In the present article we consider an hybrid setup which combines a beta-beam with an electron capture beam by using boosted Ytterbium ions. We study the sensitivity to the CP-violating phase delta and the theta_{13} angle, the CP-discovery potential …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElectron captureHigh Energy Physics::PhenomenologyPhase (waves)FOS: Physical sciencesFísica01 natural sciences7. Clean energyIonHigh Energy Physics - PhenomenologyCP violationHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino PhysicsHigh Energy Physics::ExperimentSensitivity (control systems)Neutrino010306 general physicsElectron neutrinoBeam (structure)Lepton
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Solar Neutrino Masses and Mixing from Bilinear R-Parity Broken Supersymmetry: Analytical versus Numerical Results

2003

We give an analytical calculation of solar neutrino masses and mixing at one-loop order within bilinear R-parity breaking supersymmetry, and compare our results to the exact numerical calculation. Our method is based on a systematic perturbative expansion of R-parity violating vertices to leading order. We find in general quite good agreement between approximate and full numerical calculation, but the approximate expressions are much simpler to implement. Our formalism works especially well for the case of the large mixing angle MSW solution (LMA-MSW), now strongly favoured by the recent KamLAND reactor neutrino data.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSolar neutrinoHigh Energy Physics::PhenomenologyFOS: Physical sciencesBilinear interpolationFeynman graphSupersymmetry01 natural sciencesFormalism (philosophy of mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-parity0103 physical sciencesBibliographyReactor neutrino010306 general physics
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Spontaneous R-parity violation: Lightest neutralino decays and neutrino mixing angles at future colliders

2008

We study the decays of the lightest supersymmetric particle (LSP) in models with spontaneously broken R-parity. We focus on the two cases that the LSP is either a bino or a neutral singlet lepton. We work out the most important phenomenological differences between these two scenarios and discuss also how they might be distinguished from explicit R-Parity breaking models. In both cases we find that certain ratios of decay branching ratios are correlated with either the solar or the atmospheric (and reactor) neutrino angle. The hypothesis that spontaneous R-Parity violation is the source of the observed neutrino masses is therefore potentially testable at the LHC.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSolar neutrinoHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaWeinberg angle7. Clean energy01 natural sciencesLightest Supersymmetric ParticleNuclear physicsParticle decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-parity0103 physical sciencesNeutralinoHigh Energy Physics::ExperimentNeutrino010306 general physicsLepton
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Neutrino energy reconstruction and the shape of the charged current quasielastic-like total cross section

2012

We show that because of the multinucleon mechanism effects, the algorithm used to reconstruct the neutrino energy is not adequate when dealing with quasielastic-like events, and a distortion of the total flux-unfolded cross-section shape is produced. This amounts to a redistribution of strength from high to low energies, which gives rise to a sizable excess (deficit) of low (high) energy neutrinos. This distortion of the shape leads to a good description of the MiniBooNE unfolded charged current quasielastic-like cross sections published by A. A. Aguilar-Arevalo et al. [(MiniBooNE Collaboration), Phys. Rev. D 81, 092005 (2010)]. However, these changes in the shape are artifacts of the unfol…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSolar neutrinoMany-body theoryFísicaSolar neutrino problem01 natural sciencesNuclear physicsMiniBooNE0103 physical sciencesMeasurements of neutrino speedNeutrino010306 general physicsNeutrino oscillationCharged current
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Energy-independent new physics in the flavour ratios of high-energy astrophysical neutrinos

2010

We have studied the consequences of breaking the CPT symmetry in the neutrino sector, using the expected high-energy neutrino flux from distant cosmological sources such as active galaxies. For this purpose we have assumed three different hypotheses for the neutrino production model, characterised by the flavour fluxes at production phi(0)(e) : phi(0)(mu) : phi(0)(tau) = 1 : 2 : 0, 0 : 1 : 0, and 1 : 0 : 0, and studied the theoretical and experimental expectations for the muon-neutrino flux at Earth, phi(mu), and for the flavour ratios at Earth, R = phi(mu)/phi(e) and S = phi(tau)/phi(mu). CPT violation (CPTV) has been implemented by adding an energy-independent term to the standard neutrin…

PhysicsNuclear and High Energy PhysicsParticle physicsActive galactic nucleusCPT symmetryPhysics beyond the Standard ModelFísicaFOS: Physical sciencesSeparable spacesymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Astrophysical neutrinossymbolsLarge deviations theoryCPT violationNeutrinoHamiltonian (quantum mechanics)Neutrino oscillation
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Do observations prove that cosmological neutrinos are thermally distributed?

2005

It is usually assumed that relic neutrinos possess a Fermi-Dirac distribution, acquired during thermal equilibrium in the Early Universe. However, various mechanisms could introduce strong distortions in this distribution. We perform a Bayesian likelihood analysis including the first moments of the three active neutrino distributions as free parameters, and show that current cosmological observations of light element abundances, Cosmic Microwave Background (CMB) anisotropies and Large Scale Structures (LSS) are compatible with very large deviations from the standard picture. We also calculate the bounds on non-thermal distortions which can be expected from future observations, and stress th…

PhysicsNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical Phenomenamedia_common.quotation_subjectCosmic microwave backgroundDark matterAstrophysics (astro-ph)FOS: Physical sciencesFísicaAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsUniverseCosmologyCosmic neutrino backgroundHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesisNucleosynthesisNeutrinomedia_common
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Novel Scalar Boson Decays in SUSY with Broken R-Parity

1995

R parity violation can induce mixing of the supersymmetric Higgs bosons with the sneutrinos at the tree level. We study the effect of this mixing on the decays of Higgs scalars as well as sneutrinos in an effective model where the violation of R parity is included in the minimal supersymmetric model through bilinear lepton number violating superpotential terms. We show that a small violation of R parity can lead to a sizeable branching ratio for the supersymmetric Higgs boson decay mode $H \to \chi \ell$ (where $\chi$ denotes an electroweak gaugino and $\ell$ is either a tau neutrino or a tau lepton). Relevant constraints on R parity violation as well as those coming from SUSY particle sear…

PhysicsNuclear and High Energy PhysicsParticle physicsBranching fractionHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSupersymmetryLepton numberStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Tau neutrinoR-parityHiggs bosonHigh Energy Physics::ExperimentLepton
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Neutrino observatories can characterize cosmic sources and neutrino properties

2003

Neutrino telescopes that measure relative fluxes of ultrahigh-energy $\nu_{e}, \nu_{\mu}, \nu_{\tau}$ can give information about the location and characteristics of sources, about neutrino mixing, and can test for neutrino instability and for departures from CPT invariance in the neutrino sector. We investigate consequences of neutrino mixing for the neutrino flux arriving at Earth, and consider how terrestrial measurements can characterize distant sources. We contrast mixtures that arise from neutrino oscillations with those signaling neutrino decays. We stress the importance of measuring $\nu_{e}, \nu_{\mu}, \nu_{\tau}$ fluxes in neutrino observatories.

PhysicsNuclear and High Energy PhysicsParticle physicsCOSMIC cancer databaseCPT symmetryPhysics::Instrumentation and DetectorsSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSolar neutrino problemAstrophysicsNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)Computer Science::Databases
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Dual baseline search for muon neutrino disappearance at0.5  eV2<Δm2<40  eV2

2012

The SciBooNE and MiniBooNE collaborations report the results of a νμ disappearance search in the Δ'm2 region of 0.5-40 eV2. The neutrino rate as measured by the SciBooNE tracking detectors is used to constrain the rate at the MiniBooNE Cherenkov detector in the first joint analysis of data from both collaborations. Two separate analyses of the combined data samples set 90% confidence level (CL) limits on νμ disappearance in the 0.5-40 eV2 Δm2 region, with an improvement over previous experimental constraints between 10 and 30 eV2

PhysicsNuclear and High Energy PhysicsParticle physicsCherenkov detectorDetectorlaw.inventionNuclear physicsMiniBooNElawMuon neutrinoFermilabNeutrinoNeutrino oscillationCharged currentPhysical Review D
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