Search results for "Polar"

showing 10 items of 3817 documents

Measurement of the positron longitudinal polarization in muon decay

1981

The longitudinal polarization of the ${e}^{+}$ from ${\ensuremath{\mu}}^{+}$ decay has been measured. The spin dependence of positron-electron (Bhabha) scattering and of annihilation in flight were used as the analyzing reactions. The combined statistical and systematic error was reduced by a factor of approximately 3 below that of any previous measurement. The longitudinal polarization was found to be 1.010\ifmmode\pm\else\textpm\fi{}0.064 (statistical plus systematic error) and to be consistent with the prediction of the $V\ensuremath{-}A$ interaction.

PhysicsNuclear physicsSystematic errorParticle physicsAnnihilationMuonPositronScatteringHigh Energy Physics::ExperimentPolarization (waves)Physical Review D
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Comment on the Feasibility of Antiproton Polarization in LEAR by Means of the Transverse Stern-Gerlach Effect

1984

The study of polarization effects in nucleon-nucleon scattering experiments has increased considerably our understanding of the Nuclear forces. Correspondingly it can be expected that the study of polarization phenomena in antiproton-nucleon scattering will also help us to resolve — at least partly — the complicated spin structure of the antiproton-nucleon amplitudes.

PhysicsNuclear physicsTransverse planeAmplitudeStern–Gerlach experimentAntiprotonScatteringNuclear TheoryNuclear forceSpin structureNuclear ExperimentPolarization (waves)
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The Mainz Microtron MAMI

2008

An overview of the Mainz Microtron MAMI is given. The main goal is to study the low-energy structure of hadrons. Typical examples are measurements of nucleon form factors, the polarizability of nucleons and pions and the detailed study of the excitation spectrum of nucleons. At present, an energy upgrade to 1.5 GeV (MAMI C) is close to completion. The status of the new accelerator section (HDSM) and experimental setups are briefly described and an outlook to the planned physics program is given.

PhysicsNuclear physicsUpgradePionPolarizabilityNuclear TheoryHadronNuclear ExperimentNucleonMicrotron
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Asymmetries in elastic scattering of 100 MeVπ+from a polarizedHe3target

1991

We report the observation of a large asymmetry in the elastic scattering of 100 MeV {pi}{sup +} from a polarized {sup 3}He target. Measurements have been made at laboratory angles of 60{degree}, 80{degree}, and 100{degree}, with the largest value {ital A}{sub {ital y}}=0.89{plus minus}0.12 occurring at 80{degree}, near a cross-section minimum. This asymmetry is the largest observed to date in pion scattering from a spin-1/2 nucleus. The {ital A}{sub {ital y}} data are qualitatively reproduced by a schematic model; however, agreement with the data is significantly improved when realistic three-body Faddeev wave functions and a full nonlocal distorted-wave impulse approximation reaction model…

PhysicsNuclear reactionElastic scatteringFaddeev equationsScatteringmedia_common.quotation_subjectGeneral Physics and AstronomyPolarization (waves)AsymmetryNuclear physicsPionAtomic physicsWave functionmedia_commonPhysical Review Letters
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Components of polarization-transfer to a bound proton in a deuteron measured by quasi-elastic electron scattering

2018

We report the first measurements of the transverse (Px and Py) and longitudinal (Pz) components of the polarization transfer to a bound proton in the deuteron via the H2(e→,e′p→) reaction, over a wide range of missing momentum. A precise determination of the electron beam polarization reduces the systematic uncertainties on the individual components to a level that enables a detailed comparison to a state-of-the-art calculation of the deuteron using free-proton electromagnetic form factors. We observe very good agreement between the measured and the calculated Px/Pz ratios, but deviations of the individual components. Our results cannot be explained by medium modified electromagnetic form f…

PhysicsNuclear reactionNuclear and High Energy PhysicsProton010308 nuclear & particles physicsScatteringHadronNuclear TheoryFOS: Physical sciencesElectronPolarization (waves)7. Clean energy01 natural scienceslcsh:QC1-999Deuterium0103 physical sciencespolarization-transfer ; deutronAtomic physicsNuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear ExperimentNuclear Experimentlcsh:PhysicsPhysics Letters
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Muon capture in a general class of weak models.

1985

We study muon capture by /sup 12/C in a general class of weak models. There is always a parameter characteristic of the weak model that can be extracted in a nuclear-model-independent way from the average polarization P/sub av/, the longitudinal polarization P/sub L//sup N/ and the asymmetry ..cap alpha.. in the angular distribution of recoils. For a less general class of models the asymmetry ..cap alpha.. is unnecessary. Using the experimental values of P/sub L//sup N/ and P/sub av/ we get a lower bound for the mass of the right-handed gauge boson of the left-right-symmetric model, M/sub W//sub R/> or =2.5ML, in a nuclear-model-independent way. The dependence of this bound on the experimen…

PhysicsNuclear reactionParticle physicsGauge bosonAngular momentummedia_common.quotation_subjectFísicaIsotopes of boronPolarization (waves)Upper and lower boundsAsymmetryMuon captureNuclear physicsmedia_commonPhysical review. D, Particles and fields
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Global polarization of Λ and Λ¯ hyperons in Pb-Pb collisions at sNN= 2.76 and 5.02 TeV

2020

The global polarization of the $\Lambda$ and $\overline\Lambda$ hyperons is measured for Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 and 5.02 TeV recorded with the ALICE at the LHC. The results are reported differentially as a function of collision centrality and hyperon's transverse momentum ($p_{\rm{T}}$) for the range of centrality 5-50%, $0.5 < p_{\rm{T}} <5$ GeV/$c$, and rapidity $|y|<0.5$. The hyperon global polarization averaged for Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 and 5.02 TeV is found to be consistent with zero, $\langle P_{\rm{H}}\rangle$ (%) $\approx$ 0.01 $\pm$ 0.06 (stat.) $\pm$ 0.03 (syst.) in the collision centrality range 15-50%, where the largest signal i…

PhysicsNuclear reactionParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyExtrapolationHyperonPolarization (waves)Lambda01 natural sciences0103 physical sciencesHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsCentralityPhysical Review C
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Photoproduction of π 0 mesons off protons and neutrons in the second and third nucleon resonance regions

2018

Photoproduction of mesons off quasi-free nucleons bound in the deuteron allows to study the electromagnetic excitation spectrum of the neutron and the isospin structure of the excitation of nucleon resonances. The database for such reactions is much more sparse than for free proton targets. Single $\pi^0$ photoproduction off quasi-free nucleons from the deuteron was experimentally studied. Nuclear effects were investigated by a comparison of the results for free protons and quasi-free protons and used as a correction for the quasi-free neutron data. The experiment was performed at the tagged photon beam of the Mainz MAMI accelerator for photon energies between 0.45~GeV and 1.4~GeV, using an…

PhysicsNuclear reactionProtonMeson010308 nuclear & particles physicsHadronNuclear Theory7. Clean energy01 natural sciences3. Good healthNuclear physicsPionIsospin0103 physical sciencestagged photon spectrometer ; polarization observable E ; cross-sections ; pion-photoproduction ; baryon resonances ; deuteron ; MAMI ; asymmetry ; microtron ; thresholdNeutronddc:530010306 general physicsNucleonNuclear ExperimentNuclear Experiment
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Generation of vector dark-soliton trains by induced modulational instability in a highly birefringent fiber

1999

International audience; We present a set of experimental observations that demonstrate the generation of vector trains of dark-soliton pulses in the orthogonal axes of a highly birefringent optical fiber. We generated dark-soliton trains with terahertz repetition rate in the normal group-velocity dispersion regime by inducing a polarization modulational instability by mixing two intense, orthogonal continuous laser beams. Numerical solutions of the propagation equations were used to optimize the emission of vector dark pulses at the fiber output.

PhysicsOptical fiberBirefringence[SPI.OPTI] Engineering Sciences [physics]/Optics / Photonicbusiness.industryTerahertz radiationOptical communicationPhysics::OpticsStatistical and Nonlinear PhysicsPolarization (waves)01 natural sciencesAtomic and Molecular Physics and Opticslaw.invention010309 opticsModulational instabilityOpticsOrthogonal coordinateslaw0103 physical sciences[SPI.OPTI]Engineering Sciences [physics]/Optics / Photonic[ SPI.OPTI ] Engineering Sciences [physics]/Optics / Photonic010306 general physicsbusinessLaser beams
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Modulational Instability and Stimulated Raman Scattering in Normally Dispersive Highly Birefringent Fibers

2001

Abstract The nonlinear interaction of two laser beams in normally dispersive highly birefringent optical fibers leads to a large set of fascinating physical effects such as modulational instability (MI) and stimulated Raman scattering (SRS). These two nonlinear phenomena have a positive role as a mechanism for the generation of short optical pulses and represent a drawback in fiber-optics transmissions. Indeed, we will show that an induced process of modulational instability may be exploited for the generation of THz train of vector dark solitons. The technique of frequency-resolved optical gating is used to completely characterize the intensity and phase of the dark soliton trains. On the …

PhysicsOptical fiberBirefringencebusiness.industryOrthogonal polarization spectral imagingTerahertz radiationPhase (waves)Physics::OpticsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionsymbols.namesakeModulational instabilityOpticsControl and Systems EngineeringlawsymbolsSolitonElectrical and Electronic EngineeringbusinessInstrumentationRaman scatteringOptical Fiber Technology
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