Search results for "ponte"

showing 10 items of 45 documents

Search for heavy neutral lepton production in K+ decays

2018

A search for heavy neutral lepton production in $K^+$ decays using a data sample collected with a minimum bias trigger by the NA62 experiment at CERN in 2015 is reported. Upper limits at the $10^{-7}$ to $10^{-6}$ level are established on the elements of the extended neutrino mixing matrix $|U_{\ell 4}|^2$ ($\ell=e,\mu$) for heavy neutral lepton mass in the range $170-448~{\rm MeV}/c^2$. This improves on the results from previous production searches in $K^+$ decays, setting more stringent limits and extending the mass range.

Nuclear and High Energy PhysicsleptonPontecorvo–Maki–Nakagawa–Sakata matrixheavy neutral leptons neutrino mixingFOS: Physical sciencesk mesonNA62 experiment01 natural sciencesneutrino mixingSettore FIS/04 - Fisica Nucleare e SubnuclearedecayHigh Energy Physics - ExperimentNuclear physicsneutrinoHigh Energy Physics - Experiment (hep-ex)Minimum biasEconomicaBounds; neutrinos; masses; testsTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesheavy neutral leptonslepton k meson decay neutrino010306 general physicsNuclear ExperimentPhysicsRange (particle radiation)Large Hadron Collider010308 nuclear & particles physicshep-exHigh Energy Physics::PhenomenologyAmbientalelcsh:QC1-999High Energy Physics::Experimentlcsh:PhysicsParticle Physics - ExperimentLepton
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10.8 Conclusion

2008

Nuclear physicsPhysicsHiggs fieldParticle physicsBaryon asymmetryPontecorvo–Maki–Nakagawa–Sakata matrixCP violationCosmology
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Analysis of the Lepton Mixing Matrix from Neutrino Oscillation Experiments

1988

An analysis of experimental results in the framework of simultaneous oscillations of three neutrino flavours is used, in a combined fit, to constrain the elements of the 3×3 unitary lepton mixing matrix and to obtain limits on the three lepton mixing angles αeμ αeτ and αμτ. No evidence for mixing is found.

Nuclear physicsPhysicsParticle physicsHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLepton numberMixing (physics)Lepton
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Present Knowledge of the Lepton Mixing Matrix from Neutrino Oscillation Experiments

1986

An analysis of experimental results in the framework of simultaneous oscillations of three neutrino flavours is used, in a combined fit, to constrain the elements of the 3 × 3 unitary lepton mixing matrix and to obtain limits on the three lepton mixing angles αeμ, αe τ and αμτ.

Nuclear physicsPhysicsParticle physicsSolar neutrinoHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoSolar neutrino problemNeutrino oscillationMixing (physics)Lepton
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Effects of triplet Higgs bosons in long baseline neutrino experiments

2018

The triplet scalars $(\Delta=\Delta^{++},\Delta^{+},\Delta^{0})$, utilized in the so-called Type-II seesaw model to explain the lightness of neutrinos, would generate nonstandard interactions (NSI) for neutrino propagating in matter. We investigate the prospects to probe these interactions in long baseline neutrino oscillation experiments. We analyze the upper bounds that the proposed DUNE experiment might set on the nonstandard parameters and numerically derive upper bounds, as function of the lightest neutrino mass, on the ratio the mass $M_\Delta$ of the triplet scalars and strength $|\lambda_\phi|$ of the coupling $\phi\phi\Delta$ of the triplet $\Delta$ and conventional Higgs doublet $…

Particle physicsVIOLATIONPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical scienceshiukkasfysiikkaComputer Science::Digital Libraries114 Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)effective field theory0103 physical sciences010306 general physicsNeutrino oscillationBosonPhysicsLEFT-RIGHT SYMMETRYneutrino oscillationsPARITYta114010308 nuclear & particles physicsHiggsin bosoniHigh Energy Physics::PhenomenologyneutriinotParity (physics)Coupling (probability)extensions of Higgs sectorHigh Energy Physics - PhenomenologyHiggsin bosonitHiggs bosonDOUBLY-CHARGED HIGGSHigh Energy Physics::ExperimentNeutrinoLepton
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Neutrino physics overview

2006

Seesaw-type and low-scale models of neutrino masses are reviewed, along with the corresponding structure of the lepton mixing matrix. The status of neutrino oscillation parameters as of June 2006 is given, including recent fluxes, as well as latest SNO, K2K and MINOS results. Some prospects for the next generation of experiments are given. This writeup updates the material presented in my lectures at the Corfu Summer Institute on Elementary Particle Physics in September 2005.

PhysicsHistoryParticle physicsPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesFísicaComputer Science ApplicationsEducationElementary particle physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)MINOSHigh Energy Physics::ExperimentNeutrinoNeutrino oscillation
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Predicting neutrino oscillations with “bi-large” lepton mixing matrices

2019

We propose two schemes for the lepton mixing matrix $U = U_l^\dagger U_\nu$, where $U = U_l$ refers to the charged sector, and $U_\nu$ denotes the neutrino diagonalization matrix. We assume $U_\nu$ to be CP conserving and its three angles to be connected with the Cabibbo angle in a simple manner. CP violation arises solely from the $U_l$, assumed to have the CKM form, $U_l\simeq V_{\rm CKM}$, suggested by unification. Oscillation parameters depend on a single parameter, leading to narrow ranges for the "solar" and "accelerator" angles $\theta_{12}$ and $\theta_{23}$, as well as for the CP phase, predicted as $\delta_{\rm CP}\sim 1.3\pi$.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciences01 natural scienceslcsh:QC1-999Matrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationMixing (physics)lcsh:PhysicsLeptonPhysics Letters B
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Bilarge neutrino mixing and the Cabibbo angle

2012

Recent measurements of the neutrino mixing angles cast doubt on the validity of the so-far popular tri-bimaximal mixing ansatz. We propose a parametrization for the neutrino mixing matrix where the reactor angle seeds the large solar and atmospheric mixing angles, equal to each other in first approximation. We suggest such bi-large mixing pattern as a model building standard, realized when the leading order value of the reactor angle equals the Cabibbo angle.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesFísica01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino010306 general physicsNeutrino oscillationParametrizationModel buildingMixing (physics)Ansatz
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CP Violation in the SUSY Seesaw: Leptogenesis and Low Energy

2008

We suppose that the baryon asymmetry is produced by thermal leptogenesis (with flavour effects), at temperatures $\sim 10^{9} - 10^{10}$ GeV, in the supersymmetric seesaw with universal and real soft terms. The parameter space is restricted by assuming that $l_\alpha \to l_\beta \gamma$ processes will be seen in upcoming experiments. We study the sensitivity of the baryon asymmetry to the phases of the lepton mixing matrix, and find that leptogenesis can work for any value of the phases. We also estimate the contribution to the electric dipole moment of the electron, arising from the seesaw, and find that it is (just) beyond the sensitivity of next generation experiments ($\lsim 10^{-29} e$…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixFísicaFOS: Physical sciencesSupersymmetryParameter space01 natural sciencesHigh Energy Physics - PhenomenologyElectric dipole momentBaryon asymmetryHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryLeptogenesis[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]0103 physical sciencesCP violation010306 general physics
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Lepton Flavor Violation and non-unitarity Lepton Mixing in Low-Scale Type-I Seesaw

2011

Within low-scale seesaw mechanisms, such as the inverse and linear seesaw, one expects (i) potentially large lepton flavor violation (LFV) and (ii) sizeable non-standard neutrino interactions (NSI). We consider the interplay between the magnitude of non-unitarity effects in the lepton mixing matrix, and the constraints that follow from LFV searches in the laboratory. We find that NSI parameters can be sizeable, up to percent level in some cases, while LFV rates, such as that for \mu -> e \gamma, lie within current limits, including the recent one set by the MEG collaboration. As a result the upcoming long baseline neutrino experiments offer a window of opportunity for complementary LFV and …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixInverseFOS: Physical sciencesFísica01 natural sciencesUnitary stateHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsScale typeFlavorLepton
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