Search results for "Charged current"

showing 10 items of 139 documents

"Table 16" of "A study of strange particle production in nu/mu charged current interactions in the NOMAD experiment."

2002

Efficiency corrected PT**2 distributions.

InclusiveNUMU NUCLEON --> MU- LAMBDABAR XStrange production9.266NUMU NUCLEON --> MU- KS XDeep Inelastic ScatteringSingle Differential DistributionCharged CurrentTransverse Momentum DependenceNUMU NUCLEON --> MU- LAMBDA XMuon productionDN/DPT**2
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"Table 18" of "A study of strange particle production in nu/mu charged current interactions in the NOMAD experiment."

2002

Efficiency corrected PT**2 distributions for LAMBDA production in two Feynman X regions. Note: this data does not appear in the paper.

InclusiveStrange production9.266Deep Inelastic ScatteringSingle Differential DistributionCharged CurrentTransverse Momentum DependenceNUMU NUCLEON --> MU- LAMBDA XMuon productionDN/DPT**2
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"Table 17" of "A study of strange particle production in nu/mu charged current interactions in the NOMAD experiment."

2002

Efficiency corrected PT**2 distributions for K0S production in two Feynman X regions. Note: this data does not appear in the paper.

InclusiveStrange production9.266NUMU NUCLEON --> MU- KS XDeep Inelastic ScatteringSingle Differential DistributionCharged CurrentTransverse Momentum DependenceMuon productionDN/DPT**2
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Measurement of neutrino-induced charged-current charged pion production cross sections on mineral oil atEν∼1  GeV

2011

Using a high-statistics, high-purity sample of {nu}{sub {mu}-}induced charged current, charged pion events in mineral oil (CH{sub 2}), MiniBooNE reports a collection of interaction cross sections for this process. This includes measurements of the CC{pi}{sup +} cross section as a function of neutrino energy, as well as flux-averaged single- and double-differential cross sections of the energy and direction of both the final-state muon and pion. In addition, each of the single-differential cross sections are extracted as a function of neutrino energy to decouple the shape of the MiniBooNE energy spectrum from the results. In many cases, these cross sections are the first time such quantities…

MiniBooNENuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsMuonPionMesonHigh Energy Physics::ExperimentNeutrinoEnergy sourceCharged currentLeptonPhysical Review D
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"Table 5" of "Study of D*+ production in nu/mu charged current interactions in the NOMAD experiment."

2002

Total yield of charged D* mesons per CC events.

NUMU NUCLEON --> MU- XHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryIntegrated Cross SectionDeep Inelastic ScatteringCross SectionSIGMuon productionInclusive9.266Charm productionNUMU NUCLEON --> MU- D*(2010)+ XHigh Energy Physics::ExperimentCharged CurrentNuclear Experiment
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"Table 1" of "A Precise Measurement of the Muon Neutrino-NucleonInclusive Charged Current Cross-Section off an IsoscalarTarget in the Energy Range\bo…

2007

Inclusive muon-neutrino charged current cross section.

NUMU NUCLEON --> MU- XPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyIntegrated Cross SectionDeep Inelastic ScatteringCross SectionSIGMuon productionInclusivePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentCharged Current3.084-20.716
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Neutrino interaction classification with a convolutional neural network in the DUNE far detector

2020

The Deep Underground Neutrino Experiment is a next-generation neutrino oscillation experiment that aims to measure CP-violation in the neutrino sector as part of a wider physics program. A deep learning approach based on a convolutional neural network has been developed to provide highly efficient and pure selections of electron neutrino and muon neutrino charged-current interactions. The electron neutrino (antineutrino) selection efficiency peaks at 90% (94%) and exceeds 85% (90%) for reconstructed neutrino energies between 2–5 GeV. The muon neutrino (antineutrino) event selection is found to have a maximum efficiency of 96% (97%) and exceeds 90% (95%) efficiency for reconstructed neutrino…

Neutrino Oscillations. Neutrino detectors.Physics - Instrumentation and DetectorsPhysics::Instrumentation and Detectorsfar detector01 natural sciencesPhysics Particles & FieldsHigh Energy Physics - Experimentcharged currentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Particle Physics ExperimentsMuon neutrinoneutrino/e: particle identificationNeutrino detectorsDetectors and Experimental Techniquesphysics.ins-detCharged currentneutrino: interactionInformáticaPhysicsTelecomunicacionesNeutrino oscillationsPhysicsNeutrino interactions neural network DUNE Deep Underground Neutrino ExperimentInstrumentation and Detectors (physics.ins-det)Experiment (hep-ex)Neutrino detectorPhysical SciencesCP violationNeutrinoParticle Physics - ExperimentParticle physicsdata analysis method530 Physicsneural networkAstrophysics::High Energy Astrophysical PhenomenaCONSERVATIONFOS: Physical sciencesAstronomy & AstrophysicsDeep Learningneutrino: deep underground detectorneutrino physics0103 physical sciencesNeutrino Oscillations. Neutrino detectorsObject DetectionNeutrinoCP: violationDeep Underground Neutrino ExperimentHigh Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Neutrinos010306 general physicsNeutrino oscillationneutrino/mu: particle identificationIOUScience & TechnologyDUNENeutrino interactions010308 nuclear & particles physicshep-exHigh Energy Physics::PhenomenologyFísicaNeutrino InteractionDetector530 PhysiksensitivityefficiencyHigh Energy Physics::ExperimentElectron neutrino
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One-pion production in neutrino-nucleus collisions

2013

We use our model for neutrino pion production on the nucleon to study pion production on a nucleus. The model is conveniently modified to include in-medium corrections and its validity is extended up to 2 GeV neutrino energies by the inclusion of new resonant contributions in the production process. Our results are compared with recent MiniBooNE data measured in mineral oil. Our total cross sections are below data for neutrino energies above 1 GeV. As with other theoretical calculations, the agreement with data improves if we neglect pion final state interaction. This is also the case for differential cross sections convoluted over the neutrino flux.

Nuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryFluxFOS: Physical sciences02 engineering and technology7. Clean energyResonance (particle physics)High Energy Physics - ExperimentNuclear physicsMiniBooNENuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)PionHigh Energy Physics - Phenomenology (hep-ph)0202 electrical engineering electronic engineering information engineeringNuclear ExperimentCharged currentPhysics020206 networking & telecommunicationsHigh Energy Physics - PhenomenologyDeuterium020201 artificial intelligence & image processingHigh Energy Physics::ExperimentNeutrinoNucleon
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Charged-current neutrino-nucleus scattering off the even molybdenum isotopes

2012

Neutrinos from supernovae constitute important probes of both the currently unknown supernova mechanisms and of neutrino properties. Reliable information about the nuclear responses to supernova neutrinos is therefore crucial. In this work, we compute the cross sections for the charged-current neutrino-nucleus scattering off the even-even molybdenum isotopes. The nuclear responses to supernova neutrinos are subsequently calculated by folding the cross sections with a Fermi-Dirac distribution.

Nuclear and High Energy PhysicsParticle physicsArticle SubjectPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical Phenomenachemistry.chemical_elementAstrophysics::Cosmology and Extragalactic AstrophysicsNuclear physicsmedicineCharged currentPhysicsIsotopeta114ScatteringHigh Energy Physics::Phenomenologylcsh:QC1-999Supernovamedicine.anatomical_structurechemistryTheoretical nuclear physicsMolybdenumteoreettinen ydinfysiikkaHigh Energy Physics::ExperimentNeutrinoNucleuslcsh:PhysicsAdvances in High Energy Physics
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Bose-Einstein correlations in charged current muon-neutrino interactions in the NOMAD experiment at CERN

2004

Bose-Einstein Correlations in one and two dimensions have been studied, with high statistics, in charged current muon-neutrino interaction events collected with the NOMAD detector at CERN. In one dimension the Bose-Einstein effect has been analyzed with the Goldhaber and the Kopylov-Podgoretskii phenomenological parametrizations. The Goldhaber parametrization gives the radius of the pion emission region R_G = 1.01+/-0.05(stat)+0.09-0.06(sys) fm and for the chaoticity parameter the value lambda = 0.40+/-0.03(stat)+0.01-0.06(sys). Using the Kopylov-Podgoretskii parametrization yields R_KP = 2.07+/-0.04(stat)+0.01-0.14(sys) fm and lambda_KP = 0.29+/-0.06(stat)+0.01-0.04(sys). Different paramet…

Nuclear and High Energy PhysicsParticle physicsBose-Einstein; correlations charged current; muon-neutrino interaction; NOMADHadronFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Muon neutrinoRapidity010306 general physicsNuclear ExperimentCharged currentPhysicsLarge Hadron Collider010308 nuclear & particles physicsFísicaBose–Einstein correlationsCharged particleHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsParticle Physics - Experiment
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