Search results for "PION"

showing 10 items of 1304 documents

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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Photoproduction of the f2(1270) resonance

2014

We have performed a calculation of the $\gamma p \to \pi^+ \pi^- p$ reaction, where the two pions have been separated in $D$-wave producing the $f_2(1270)$ resonance. We use elements of the local hidden gauge approach that provides the interaction of vector mesons in which the $f_2(1270)$ resonance appears as a $\rho$-$\rho$ molecular state in $L=0$ and spin 2. The vector meson dominance, incorporated in the local hidden gauge approach converts a photon into a $\rho^0$ meson and the other meson connects the photon with the proton. The picture is simple and has no free parameters, since the parameters of the theory have been constrained in the previous study of the vector-vector states. In a…

Nuclear and High Energy PhysicsParticle physicsPhotonMesonNuclear TheoryHigh Energy Physics::LatticeHadronFOS: Physical sciences01 natural sciencesResonance (particle physics)High Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)PionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentSpin-½Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPropagatorFísicaVector meson dominanceHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Evidence of Electron Neutrino Appearance in a Muon Neutrino Beam

2013

The T2K Collaboration reports evidence for electron neutrino appearance at the atmospheric mass splitting, vertical bar Delta m(32)(2)vertical bar approximate to 2.4 X 10(-3) eV(2). An excess of electron neutrino interactions over background is observed from a muon neutrino beam with a peak energy of 0.6 GeV at the Super-Kamiokande (SK) detector 295 km from the beam's origin. Signal and background predictions are constrained by data from near detectors located 280 m from the neutrino production target. We observe 11 electron neutrino candidate events at the SK detector when a background of 3.3 +/- 0.4(syst) events is expected. The background-only hypothesis is rejected with a p value of 0.0…

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsFOS: Physical sciencesFluxddc:500.201 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Momentum rangeMuon neutrino010306 general physicsNeutrino oscillationPhysics010308 nuclear & particles physicsT2K experimentFísicaHigh Energy Physics::ExperimentNeutrinoAbsorption cross-sectionsElectron neutrinoBeam (structure)
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Hadron energy reconstruction for the ATLAS calorimetry in the framework of the non-parametrical method

2002

This paper discusses hadron energy reconstruction for the ATLAS barrel prototype combined calorimeter (consisting of a lead-liquid argon electromagnetic part and an iron-scintillator hadronic part) in the framework of the non-parametrical method. The non-parametrical method utilizes only the known $e/h$ ratios and the electron calibration constants and does not require the determination of any parameters by a minimization technique. Thus, this technique lends itself to an easy use in a first level trigger. The reconstructed mean values of the hadron energies are within $\pm 1%$ of the true values and the fractional energy resolution is $[(58\pm3)% /\sqrt{E}+(2.5\pm0.3)%]\oplus (1.7\pm0.2)/E…

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsHadronFOS: Physical scienceschemistry.chemical_elementCalorimetryElectronCalorimetry01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentEnergy measurementNuclear physicsHigh Energy Physics - Experiment (hep-ex)PionShower counter0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Computer data analysis[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Combined calorimeterDetectors and Experimental Techniques010306 general physicsNuclear ExperimentInstrumentationPhysicsLarge Hadron ColliderArgon010308 nuclear & particles physicsSHOWER DEVELOPMENT; RESOLUTIONSHOWER DEVELOPMENTCalorimeterRESOLUTIONchemistryScintillation counterHigh Energy Physics::ExperimentCompensation
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Study of the response of the ATLAS central calorimeter to pions of energies from 3 to 9 GeV

2009

Çetin, Serkant Ali (Dogus Author) A fully instrumented slice of the ATLAS central detector was exposed to test beams from the SPS (Super Proton Synchrotron) at CERN in 2004. In this paper, the response of the central calorimeters to pions with energies in the range between 3 and 9 GeV is presented. The linearity and the resolution of the combined calorimetry (electromagnetic and hadronic calorimeters) was measured and compared to the prediction of a detector simulation program using the toolkit Geant 4.

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsHadronNuclear TheoryCalorimetry01 natural sciencesNuclear physicsPionAtlas (anatomy)0103 physical sciencesmedicineCalibration[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsNuclear ExperimentInstrumentationPhysicsLarge Hadron Collider010308 nuclear & particles physicsDetectorATLASSuper Proton SynchrotronCalorimetermedicine.anatomical_structureCalibrationPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentTest beamSimulation
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T2K neutrino flux prediction

2013

The Tokai-to-Kamioka (T2K) experiment studies neutrino oscillations using an off-axismuon neutrino beam with a peak energy of about 0.6 GeV that originates at the Japan Proton Accelerator Research Complex accelerator facility. Interactions of the neutrinos are observed at near detectors placed at 280 m from the production target and at the far detector-Super-Kamiokande-located 295 km away. The flux prediction is an essential part of the successful prediction of neutrino interaction rates at the T2K detectors and is an important input to T2K neutrino oscillation and cross section measurements. A FLUKA and GEANT3-based simulation models the physical processes involved in the neutrino producti…

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoAstrophysics::High Energy Astrophysical Phenomenaddc:500.2Antiprotons01 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsPions0103 physical sciencesMomentum rangeMuon neutrino010306 general physicsNeutrino oscillationNuclear ExperimentQCPhysicsGev-c010308 nuclear & particles physicsParticle-productionHigh Energy Physics::PhenomenologyT2K experimentFísicaDetectorMonitorSolar neutrino problemNucleiNeutrino detector13. Climate actionMeasurements of neutrino speedPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNeutrinoProtonsAbsorption cross-sectionsParticle 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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s-wave pion-nucleus optical potential

2007

We calculate the s-wave part of the pion-nucleus optical potential using a unitarized chiral approach that has been previously used to simultaneously describe pionic hydrogen and deuterium data as well as low energy pi N scattering in the vacuum. This energy dependent model allows for additional isoscalar parts in the potential from multiple rescattering. We consider Pauli blocking and pion polarization in an asymmetric nuclear matter environment. Also, higher order corrections of the pi N amplitude are included. The model can accommodate the repulsion required by phenomenological fits, though the theoretical uncertainties are bigger than previously thought. At the same time, we also find a…

Nuclear and High Energy PhysicsParticle physicsscattering amplitude [pi nucleon]Nuclear Theorymedia_common.quotation_subjectIsoscalarpartial waveNuclear TheoryFOS: Physical sciencesAsymmetryrenormalizationNuclear physicsNuclear Theory (nucl-th)symbols.namesakePionPauli exclusion principlemesic atom [deuterium]unitarityddc:530higher-order [Feynman graph]nuclear reaction [pi nucleus]numerical calculationsNuclear Experimentmedia_commonPhysicschiral [symmetry]UnitarityIsovectorN(1440)FísicaNuclear mattermesic atom [hydrogen]propagator [pi]Scattering amplitudenuclear mattersymbolsoptical [potential]correction [vertex function]
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Detection of charged pions and protons in the segmented electromagnetic calorimeter TAPS

1998

We present the characteristics of the segmented BaF2 calorimeter TAPS for the measurement of charged pions and protons. The method of particle identification exploits the relation between the kinetic energy of a particle, its mass and the time-of-flight required to reach the detector. The detection efficiency is calculated using GEANT-GCALOR simulations. The analysis method is applied in the reaction Ar-40 + Ca-nat at 0.8A GeV. The simultaneous detection of charged pions and protons can be used to search for correlated pairs signalling the de-excitation of the Delta(1232) resonance. (C) 1998 Elsevier Science B.V. All rights reserved.

Nuclear and High Energy PhysicsPhotonBAF2 SCINTILLATORSHEAVY-ION COLLISIONSPHOTONSKinetic energy01 natural sciencesResonance (particle physics)Particle identificationENERGYNuclear physicsPion0103 physical sciencesABSORPTIONPARTICLESNuclear Experiment010306 general physicsInstrumentationcharged pion detectionPhysicsDelta(1232) resonance detectionCalorimeter (particle physics)010308 nuclear & particles physicsDetectorproton detection[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]ParticleHigh Energy Physics::ExperimentAtomic physics
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