Search results for "Neutral Current"

showing 10 items of 301 documents

Photon emission in neutral-current interactions at intermediate energies

2013

Neutral current photon emission reactions with nucleons and nuclei are studied. These processes are important backgrounds for nu_mu to nu_e (bar(nu)_mu to bar(nu)_e) appearance oscillation experiments where electromagnetic showers instigated by electrons (positrons) and photons are not distinguishable. At intermediate energies, these reactions are dominated by the weak excitation of the Delta(1232) resonance and its subsequent decay into Ngamma There are also non-resonant contributions that, close to threshold, are fully determined by the effective chiral Lagrangian of strong interactions. In addition, we have also included mechanisms mediated by nucleon excitations (N*) from the second res…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryStrong interactionNuclear TheoryFOS: Physical sciencesElectron01 natural sciencesResonance (particle physics)High Energy Physics - ExperimentNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Experiment (hep-ex)Pauli exclusion principleHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationNuclear ExperimentPhysicsNeutral current010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics - Phenomenology13. Climate actionsymbolsHigh Energy Physics::ExperimentNeutrinoAtomic physicsNucleon
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Can One Distinguish Tau Neutrinos from Antineutrinos in Neutral-Current Pion Production Processes?

2007

A potential way to distinguish tau-neutrinos from antineutrinos, below the tau-production threshold, but above the pion production one, is presented. It is based on the different behavior of the neutral current pion production off the nucleon, depending on whether it is induced by neutrinos or antineutrinos. This procedure for distinguishing tau-neutrinos from antineutrinos neither relies on any nuclear model, nor it is affected by any nuclear effect (distortion of the outgoing nucleon waves, etc...). We show that neutrino-antineutrino asymmetries occur both in the totally integrated cross sections and in the pion azimuthal differential distributions. To define the asymmetries for the latte…

Nuclear and High Energy PhysicsParticle physicsNuclear Theorymedia_common.quotation_subjectNuclear TheoryFOS: Physical sciencesAsymmetryHigh Energy Physics - ExperimentNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)PionHigh Energy Physics - Phenomenology (hep-ph)Nuclear Experimentmedia_commonPhysicsMuonNeutral currentHigh Energy Physics::PhenomenologyFísicaMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoNucleonLepton
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A Search for Single Photon Events in Neutrino Interactions

2011

We present a search for neutrino induced events containing a single, exclusive photon using data from the NOMAD experiment at the CERN SPS where the average energy of the neutrino flux is ≃25 GeV. The search is motivated by an excess of electron-like events in the 200-475 MeV energy region as reported by the MiniBooNE experiment. In NOMAD, photons are identified via their conversion to e + e - in an active target embedded in a magnetic field. The background to the single photon signal is dominated by the asymmetric decay of neutral pions produced either in a coherent neutrino-nucleus interaction, or in a neutrino-nucleon neutral current deep inelastic scattering, or in an interaction occurr…

Nuclear and High Energy PhysicsParticle physicsPhotonFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsMiniBooNENeutral currentHigh Energy Physics - Experiment (hep-ex)PionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Coherent; Neutral current; Neutrino; Pion; Single photon; Nuclear and High Energy Physics010306 general physicsCharged currentPhysicsSingle photon; Neutrino; Neutral current; Coherent; PionNeutral current010308 nuclear & particles physicsFísicaDeep inelastic scatteringsingle photon; neutrino; neutral current; coherent; pionHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]PionHigh Energy Physics::ExperimentSingle photonNeutrinoCoherentEvent (particle physics)Particle Physics - Experiment
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Photon emission in neutral current interactions at the T2K experiment

2015

9 pages.- 6 figures

Nuclear and High Energy PhysicsParticle physicsPhotonNuclear TheoryPhysics::Instrumentation and DetectorsFOS: Physical sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsMiniBooNENuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Event generatorPhysicsNeutral currentHigh Energy Physics::PhenomenologyT2K experimentFísicaMinibooneHigh Energy Physics - PhenomenologyCP violationHigh Energy Physics::ExperimentNeutrinoCross-sectionsNucleon
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A measurement of the inclusive b → sγ branching ratio

1998

The flavour changing neutral current decay b --> s gamma has been detected in hadronic Z decays collected by ALEPH at LEP. The signal is isolated in lifetime-tagged b (b) over bar events by the presence of a hard photon associated with a system of high momentum and high rapidity hadrons. The background processes are normalised from the data themselves. The inclusive branching ratio is measured to be (3.11 +/- 0.80(stat) +/- 0.72(syst)) x 10(-4), consistent with the Standard Model expectation via penguin processes. (C) 1998 Published by Elsevier Science B.V. All rights reserved. The flavour changing neutral current decay b → sγ has been detected in hadronic Z decays collected by ALEPH at …

Nuclear and High Energy PhysicsParticle physicsPhotonelectron positron. colliding beamselectron positron. annihilationElectron–positron annihilationquark. pair productionHadronlepStandard ModelquarkALEPH ExperimentNuclear physicsRapidityALEPH experimentPhysicselectron positronNeutral currentquark. radiative decayBranching fractionPhysicsHigh Energy Physics::PhenomenologyALEPH Experiment; lepquark. branching ratioHigh Energy Physics::Experimentexperimental results
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New global fits to $b \to s$ data with all relevant parameters

2018

The LHCb experiment has made several measurements in $b \to s$ transitions which indicate tensions with the Standard Model predictions. Assuming the source of these tensions to be new physics, we present new global fits to all Wilson coefficients which can effectively receive beyond the Standard Model contributions. While the theoretically clean ratios $R_{K^{(*)}}$ which are sensitive to lepton flavour non-universality may unambiguously establish lepton non-universal new physics in the near future, most of the other tensions with the SM in the $b \to s$ data, in particular in the angular observables of the $B\to K^* \mu\mu$ decay and in the branching ratio of the $B_s \to \phi \mu\mu$ deca…

Nuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeFlavourFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesdecay: flavor changingB --> K muon+ muon-010306 general physicsB: rare decayParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsnew physicsneutral current: flavor changinghep-phObservableLHC-BB: branching ratio: ratioB --> K*(892) muon+ muon-High Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentflavor: violationB/s --> Phi(1020) muon+ muon-Lepton
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Prediction of neutrino fluxes in the NOMAD experiment

2003

The method developed for the calculation of the flux and composition of the West Area Neutrino Beam used by NOMAD in its search for neutrino oscillations is described. The calculation is based on particle production rates computed using a recent version of FLUKA and modified to take into account the cross sections measured by the SPY and NA20 experiments. These particles are propagated through the beam line taking into account the material and magnetic fields they traverse. The neutrinos produced through their decays are tracked to the NOMAD detector. The fluxes of the four neutrino flavours at NOMAD are predicted with an uncertainty of about 8% for nu(mu) and nu(e), 10% for antinu(mu), and…

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciences01 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNeutrino oscillationInstrumentationCharged currentPhysicsNeutral current010308 nuclear & particles physicsDetectorHigh Energy Physics::PhenomenologyFísicaSolar neutrino problemMagnetic fieldBeamlineHigh Energy Physics::ExperimentNeutrinoParticle Physics - Experiment
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How strange is pion electroproduction?

2015

We consider pion production in parity-violating electron scattering (PVES) in the presence of nucleon strangeness in the framework of partial wave analysis with unitarity. Using the experimental bounds on the strange form factors obtained in elastic PVES, we study the sensitivity of the parity-violating asymmetry to strange nucleon form factors. For forward kinematics and electron energies above 1 GeV, we observe that this sensitivity may reach about 20\% in the threshold region. With parity-violating asymmetries being as large as tens p.p.m., this study suggests that threshold pion production in PVES can be used as a promising way to better constrain strangeness contributions. Using this m…

Nuclear and High Energy PhysicsParticle physicsProtonNuclear Theorymedia_common.quotation_subjectPartial wave analysisNuclear TheoryFOS: Physical sciencesStrangeness01 natural sciencesAsymmetryNuclear physicsNuclear Theory (nucl-th)PionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear Experimentmedia_commonPhysicsNeutral currentUnitarity010308 nuclear & particles physicslcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNucleonlcsh:Physics
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Inclusive Nucleon Emission Induced by Quasi--Elastic Neutrino--Nucleus Interactions

2005

We study the quasi--elastic contribution to the inclusive $(\nu_l,\nu_l N)$, $(\nu_l,l^- N)$, $({\bar \nu}_l,{\bar \nu}_l N)$ and $({\bar \nu}_l,l^+ N)$ reactions in nuclei using a Monte Carlo simulation method to account for the rescattering of the outgoing nucleon. As input, we take the reaction probability from the microscopical many body framework developed in Phys. Rev. {\bf C70} (2004) 055503 for charged-current induced reactions, while for neutral currents we use results from a natural extension of the model described in that reference. The nucleon emission process studied here is a clear signal for neutral--current neutrino driven reactions, that can be used in the analysis of futur…

Nuclear reactionPhysicsParticle physicsNuclear and High Energy PhysicsNeutral currentNuclear TheoryNeutron emissionMonte Carlo methodNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsNuclear Theory (nucl-th)Nuclear physicsMany-body problemHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoRandom phase approximationNucleonNuclear Experiment
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Search for flavor-changing neutral current and lepton-flavor violating decays of D-0 -> l(+)l(-)

2004

We report on a search for the flavor-changing neutral current decays $\Dz\to e^+e^-$ and $\Dz\to\mu^+\mu^-$, and the lepton-flavor violating decay $\Dz\to e^\pm\mu^\mp$. The measurement is based on $122 {fb}^{-1}$ of data collected by the \babar detector at the PEP-II asymmetric $e^+e^-$ collider. No evidence is found for any of the decays. The upper limits on the branching fractions, at the 90 % confidence level, are $1.2\times 10^{-6}$ for $\Dz\to e^+e^-$, $1.3\times 10^{-6}$ for $\Dz\to\mu^+\mu^-$, and $8.1\times 10^{-7}$ for $\Dz\to e^\pm\mu^\mp$.

OptimizationParticle physicsLepton-flavor violating (LFV)Electron–positron annihilationBABARCharged particleGeneral Physics and Astronomy-Standard model (SM)Lambda baryon01 natural sciencesPARTICLE PHYSICS; PEP2; BABARHigh Energy Physics - ExperimentNONuclear physicsSilicon microstrip detector0103 physical sciencesPEP2010306 general physicsDETECTOR; BABAR; SLACDETECTORFlavorProbabilityPhysicsNeutral current010308 nuclear & particles physicsEnergy dissipationFlavor-changing neutral currentColliding beam acceleratorMicrostrip deviceHEPFlavor-changing neutral current (FCNC)Drift chamberPARTICLE PHYSICSHigh Energy Physics::ExperimentParticle detectorSLACLepton
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