Search results for "Nucleon"

showing 10 items of 1041 documents

"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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Mesure de la section efficace de l'électroproduction de photons à JLAB dans le but d'effectuer une Séparation Rosenbluth de la contribution DVCS

2014

The study of the inner structure of hadrons allows us to understand the nature of the interactions between partons, quarks and gluons, described by Quantum Chromodynamics. The elastic scattering reactions, which have been studied in order to measure the nucleon form factors, are included in this frame. The inelastic scattering reactions are also included in this frame, they allow us to obtain information about the nucleon structure thanks to the development of the parton distribution functions (PDFs). While through elastic scattering we can obtain information about the charge distribution of the nucleon, and hence, about the spatial distribution of the partons, through inelastic scattering …

Jefferson Lab (CEBAF)Réactions exclusivesDeeply Virtual Compton Scattering (DVCS)Structure du nucléonNucleon structureElectromagnetic probefísica de partículasGeneralized Parton Distributions (GPDs)Exclusive reactions[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Diffusion Compton Profondément Virtuelle (DVCS)Sonde électromagnétiqueHigh Energy Physics::Experimentfísica de altas energíasNuclear ExperimentDistributions de partons généralisées (GPDs)
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Accessing the gluonic structure of light nuclei at a future electron-ion collider

2020

We show how exclusive vector meson production off light ions can be used to probe the spatial distribution of small-$x$ gluons in the deuteron and $^3$He wave functions. In particular, we demonstrate how short range repulsive nucleon-nucleon interactions affect the predicted coherent $J/\Psi$ production spectra. Fluctuations of the nucleon substructure are shown to have a significant effect on the incoherent cross section above $|t|\gtrsim 0.2\,\mathrm{GeV}^2$. By explicitly performing the JIMWLK evolution, we predict the $x$-dependence of coherent and incoherent cross sections in the EIC energy range. Besides the increase of the average size of the nucleus with decreasing $x$, both the gro…

Length scaleCOLLISIONSProtonNuclear TheoryNuclear TheoryElectronhiukkasfysiikkaPROTON01 natural sciences114 Physical sciencesComputer Science::Digital LibrariesNuclear physicsP PLUS P0103 physical sciencesSaturation (graph theory)EQUATIONVector meson010306 general physicsNuclear ExperimentSCALEPhysics010308 nuclear & particles physicsFLUCTUATIONSGluonHigh Energy Physics - PhenomenologySATURATIONydinfysiikkaNucleonColor chargePhysical Review C
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Measurement of the Generalized Polarizabilities of the Proton at Intermediate $Q^2$

2021

Background: Generalized polarizabilities (GPs) are important observables to describe the nucleon structure, and measurements of these observables are still scarce. Purpose: This paper presents details of a virtual Compton scattering (VCS) experiment, performed at the A1 setup at the Mainz Microtron by studying the $e p \to e p \gamma$ reaction. The article focuses on selected aspects of the analysis. Method: The experiment extracted the $P_{LL} -P_{TT} / \epsilon$ and $P_{LT}$ structure functions, as well as the electric and magnetic GPs of the proton, at three new values of the four-momentum transfer squared $Q^2$: 0.10, 0.20 and 0.45 GeV$^2$. Results: We emphasize the importance of the ca…

MAINZ-A1ProtonNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]higher-orderHadronic Physics and QCDFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]momentum transfer dependence01 natural scienceselectron p: scatteringNuclear Theory (nucl-th)Cross section (physics)High Energy Physics - Phenomenology (hep-ph)Polarizability0103 physical sciencesCalibrationp: structure functionNuclear Experiment (nucl-ex)010306 general physicsMicrotronNuclear ExperimentPhysics010308 nuclear & particles physicsCompton scatteringObservablecross section: measuredcalibrationComputational physicsHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]p: polarizabilityelectron p --> electron p photonNucleonCompton scatteringexperimental results
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Tensor Analyzing Powers for Quasi-Elastic Electron Scattering from Deuterium

1999

We report on a first measurement of tensor analyzing powers in quasi-elastic electron-deuteron scattering at an average three-momentum transfer of 1.7 fm$^{-1}$. Data sensitive to the spin-dependent nucleon density in the deuteron were obtained for missing momenta up to 150 MeV/$c$ with a tensor polarized $^2$H target internal to an electron storage ring. The data are well described by a calculation that includes the effects of final-state interaction, meson-exchange and isobar currents, and leading-order relativistic contributions.

MOMENTUM DISTRIBUTIONNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesElectron01 natural scienceslaw.inventionNuclear physicslawNUCLEON CROSS-SECTIONS0103 physical sciencesTensorSTORAGE-RINGNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsFORM-FACTORPOLARIZED ELECTRONS010308 nuclear & particles physicsScatteringParticle accelerator3. Good healthTARGETDeuteriumIsobarNEUTRONNucleonElectron scattering
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"Table 1" of "Exclusive rho0 and phi muoproduction at large q**2"

1995

No description provided.

MUON DEUT --> MUON RHO0 DEUTGAMMA* NUCLEON --> RHO0 NUCLEONPhotoproductionIntegrated Cross SectionExclusiveCross SectionSIGMuon production19.393
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"Table 5" of "Exclusive rho0 and phi muoproduction at large q**2"

1995

No description provided.

MUON NUCLEUS --> C MUON RHO0GAMMA* NUCLEON --> RHO0 NUCLEONPhotoproductionMUON C --> MUON RHO0 CIntegrated Cross SectionExclusiveCross SectionSIGMuon production19.393
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"Table 2" of "Exclusive rho0 and phi muoproduction at large q**2"

1995

No description provided.

MUON NUCLEUS --> C MUON RHO0GAMMA* NUCLEON --> RHO0 NUCLEONPhotoproductionMUON C --> MUON RHO0 CIntegrated Cross SectionExclusiveCross SectionSIGMuon production19.393
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"Table 3" of "Exclusive rho0 and phi muoproduction at large q**2"

1995

No description provided.

MUON NUCLEUS --> CA MUON RHO0GAMMA* NUCLEON --> RHO0 NUCLEONPhotoproductionIntegrated Cross SectionExclusiveMUON CA --> MUON RHO0 CACross SectionSIGMuon production19.393
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