Search results for "Structure Function"

showing 10 items of 177 documents

"Table 2" of "Study of Dimuon Production in Photon-Photon Collisions and Measurement of QED Photon Structure Functions at LEP"

2001

The measured QED photon structure function at Q**2 = 120 GeV for the combine SAT and STIC data.

GAMMA GAMMA --> MU+ MU-Electron productionE+ E- --> E+ E- MU+ MU-91.2Computer Science::Computational ComplexityMuon productionF2PhotoproductionE+ E- ScatteringTwo-PhotonStructure FunctionExclusiveHigh Energy Physics::ExperimentPhysics::Atomic PhysicsNuclear Experiment
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A glimpse of gluons through deeply virtual compton scattering on the proton

2017

The internal structure of nucleons (protons and neutrons) remains one of the greatest outstanding problems in modern nuclear physics. By scattering high-energy electrons off a proton we are able to resolve its fundamental constituents and probe their momenta and positions. Here we investigate the dynamics of quarks and gluons inside nucleons using deeply virtual Compton scattering (DVCS)—a highly virtual photon scatters off the proton, which subsequently radiates a photon. DVCS interferes with the Bethe-Heitler (BH) process, where the photon is emitted by the electron rather than the proton. We report herein the full determination of the BH-DVCS interference by exploiting the distinct energ…

Genetics and Molecular Biology (all)PhotonProtonHigh Energy Physics::LatticeNuclear TheoryGeneral Physics and AstronomyVirtual particleparton: distribution functionBiochemistry01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]p: structure functionNuclear Experiment (nucl-ex)[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]lcsh:ScienceNuclear ExperimentNuclear ExperimentPhysicsenergy: highMultidisciplinarystrong interactionChemistry (all)QCompton scattering: form factorphoton: energy spectrumHigh Energy Physics - Phenomenologyconfinementelectron p --> electron p photonchannel cross section: measuredQuarkelectron p: deep inelastic scatteringParticle physicselectron: polarized beamScienceStrong interactionFOS: Physical sciencesBethe-Heitler[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ArticleGeneral Biochemistry Genetics and Molecular Biologyenergy dependencequarkPhysics and Astronomy (all)[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]photon: emissiondeeply virtual Compton scattering0103 physical sciencesstructure010306 general physicsquantum mechanics: interference010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCompton scatteringGeneral ChemistrygluonsensitivityGluon[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quark–gluon plasmalcsh:Q[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentholographyChemistry (all); Biochemistry Genetics and Molecular Biology (all); Physics and Astronomy (all)photon: virtualexperimental results
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Structure function as a tool in AE and Dst time series analysis

1995

A new method to analyse the structure function (SF) has been constructed and used in the analysis of the AE time series for the years 1978-85 and Dst time series for 1957-84. It is shown that this SF analysis makes a clear distinction between affine and periodicity dominated time series, and it displays the essential periodicities of the series in a range relevant to its characteristic time scale. The AE time series is found to be affine such that the scaling exponent changes at a time scale of 113 (±9) minutes. On the other hand, in the SF function analysis, the Dst data are dominated by the 24-hour and 27-day periods. The 27-day period is modulated by the annual variation.

GeophysicsSeries (mathematics)Scale (ratio)Structure functionExponentRange (statistics)General Earth and Planetary SciencesStatistical physicsAffine transformationTime seriesScalingMathematicsGeophysical Research Letters
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Hepatitis B core particles as a universal display model: a structure-function basis for development

1999

AbstractBecause it exhibits a remarkable capability to accept mutational intervention and undergo correct folding and self-assembly in all viable prokaryotic and eukaryotic expression systems, hepatitis B core (HBc) protein has been favored over other proposed particulate carriers. Structurally, the unusual α-helical organization of HBc dimeric units allows introduction of foreign peptide sequences into several areas of HBc shells, including their most protruding spikes. Progress toward full resolution of the spatial structure as well as accumulation of chimeric HBc-based structures has brought closer the knowledge-based design of future vaccines, gene therapy tools and other artificial par…

Hepatitis B virusGenes ViralCryo-electron microscopyMacromolecular SubstancesProtein ConformationBiophysicsComputational biologyBiologyBiochemistryMolecular displayEpitopesProtein structureStructural BiologyGeneticsProkaryotic expressionAnimalsHumansMolecular BiologyDrug CarriersBinding SitesSpatial structureViral Core ProteinsStructure functionHepatitis B core proteinvirus diseasesCell BiologyBasis (universal algebra)Self-assemblyAntigenicityVirologyBiological EvolutionHepatitis B Core Antigensdigestive system diseasesFolding (chemistry)Protein structureElectron cryomicroscopyDimerizationHepatitis b coreFEBS Letters
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Spectroscopy of short-lived radioactive molecules: A sensitive laboratory for new physics

2019

The study of molecular systems provides exceptional opportunities for the exploration of the fundamental laws of nature and for the search for physics beyond the Standard Model of particle physics. Measurements of molecules composed of naturally occurring nuclei have provided the most stringent upper bounds to the electron electric dipole moment to date, and offer a route to investigate the violation of fundamental symmetries with unprecedented sensitivity. Radioactive molecules - where one or more of their atoms possesses a radioactive nucleus - can contain heavy and deformed nuclei, offering superior sensitivity for EDM measurements as well as for other symmetry-violating effects. Radium …

High Energy Physics - TheoryexceptionalNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]collinearFOS: Physical sciencesnucleus: structure function[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)ionizationPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experimentenhancementnew physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]stabilitysensitivitylaserradiumelectron: electric momentHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)radioactivity[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]many-body problemnucleus: deformation
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"Table 6" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The spin-dependent structure function G1(P) evolved to Q**2=10 GeV**2.. The second systematic (DSYS) error is due to the uncertainty in the QCD evolution.

Inclusive13.729-18.903Spin Dependent Structure FunctionG1Neutral CurrentDeep Inelastic ScatteringHigh Energy Physics::ExperimentMU+ P --> MU+ XMuon production
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"Table 11" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The nonsinglet spin-dependent structure function G1(NS) evolved to Q**2=10 GeV**2.. The second systematic (DSYS) error is due to the uncertainty in the QCD evolution.

Inclusive13.729-18.903Spin Dependent Structure FunctionG1Neutral CurrentDeep Inelastic ScatteringHigh Energy Physics::ExperimentMU+ P --> MU+ XMuon productionMU+ DEUT --> MU+ X
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"Table 10" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The nonsinglet spin-dependent structure function G1(NS) calculated from themeasured the G1(P) and G1(D).

Inclusive13.729-18.903Spin Dependent Structure FunctionG1Neutral CurrentDeep Inelastic ScatteringMU+ P --> MU+ XMuon productionMU+ DEUT --> MU+ X
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"Table 5" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The spin-dependent proton structure function G1.

Inclusive13.729-18.903Spin Dependent Structure FunctionNuclear TheoryG1Neutral CurrentDeep Inelastic ScatteringPhysics::Accelerator PhysicsCondensed Matter::Strongly Correlated ElectronsNuclear ExperimentMU+ P --> MU+ XMuon production
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"Table 6" of "The spin-dependent structure function g1(x) of the deuteron from polarized deep-inelastic muon scattering."

1997

Combining with earlier measured value of G1(P).

Inclusive18.903MU+ N --> MU+ XSpin Dependent Structure FunctionG1Neutral CurrentDeep Inelastic ScatteringMU+ P --> MU+ XMuon productionMU+ DEUT --> MU+ X
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