Search results for "SPHERICITY"

showing 10 items of 34 documents

"Table 21" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Distributions of Sphericity at cm energies 133, 161 and 172 GeV.

Astrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentSingle Differential DistributionJet ProductionNuclear Experiment133.0-172.0DN/DSPHERICITY
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"Table 22" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Distribution of Sphericity at cm energy 183 GeV.

Astrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentSingle Differential DistributionJet ProductionNuclear ExperimentDN/DSPHERICITY183.0
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"Table 36" of "Properties of hadronic Z decays and test of QCD generators"

1992

Distribution of rapidity with respect to sphericity axis.

E+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringExclusive91.2Single Differential DistributionDN/DSPHERICITY
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"Table 2" of "Properties of hadronic Z decays and test of QCD generators"

1992

Sphericity distribution.

E+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringExclusive91.2Single Differential DistributionDN/DSPHERICITY
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"Table 1" of "Properties of hadronic Z decays and test of QCD generators"

1992

Sphericity distribution.

E+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringExclusive91.2Single Differential DistributionDN/DSPHERICITY
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"Table 37" of "Properties of hadronic Z decays and test of QCD generators"

1992

Distribution of rapidity with respect to sphericity axis.

E+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringExclusive91.2Single Differential DistributionDN/DSPHERICITY
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Colloquium: The Shape of Hadrons

2012

This Colloquium addresses the issue of the shape of hadrons and, in particular, that of the proton. The concept of shape in the microcosm is critically examined. Special attention is devoted to properly define the meaning of shape for bound-state systems of near massless quarks. The ideas that lead to the expectation of nonsphericity in the shape of hadrons, the calculations that predict it, and the experimental information obtained from recent high-precision measurements are examined. Particular emphasis is given to the study of the electromagnetic transition between the nucleon and its first excited state, the Δ(1232) resonance. The experimental evidence is critically examined and compare…

First excited stateQuarkQuantum chromodynamicsPhysicsParticle physicsPhenomenological modelsPhysicsEffective field theoryHadronBound stateGeneral Physics and AstronomyHadronsExperimental evidenceMassless particleBaryonElectromagnetic transitionsHigh-precision measurementNonsphericityLattice calculationsEffective field theoryBibliographyNucleonReviews of Modern Physics
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Influence of a density mismatch on TMPTMA shells nonconcentricity

2011

Some laser target designs require low-density organic foam shells to study fusion on the French high-power laser laser mega joule. Low-density trimethylolpropane trimethacrylate foam shells composed of C, H, and O, 2 mm diameter, 100-μm wall thickness, and 250 mg cm−3 density are synthesized by a microencapsulation technique using a droplet generator. These shells have to reach a sphericity higher than 99.9% and a nonconcentricity (NC) lower than 1%. The wall thickness variation is one of the most difficult specifications to meet. An important factor in reducing this defect is the density matching between the three phases of the emulsion at polymerization temperature. The influence of a den…

FusionMaterials sciencePolymers and PlasticsShell (structure)General ChemistryLaserSurfaces Coatings and Filmslaw.inventionSphericityPolymerizationlawPhase (matter)EmulsionMaterials ChemistryComposite materialDispersion (chemistry)Journal of Applied Polymer Science
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The pseudostationary mercury electrode

1998

Abstract A detailed study of the pseudostationary mercury electrode is presented, based on its use in LSV. Delay times ( t 1 ) as short as 20 ms can be employed; the drop area is still given by its classical expression, and minimization of the ohmic drop allows sweep rates of a few thousands of volts per second to be used. The conditions for pseudostationarity are given; the lower sweep rates utilizable are of the order of few tenths of volt per second. Reactant adsorption is considered, and zones where rehomogenization near the electrode surface is practically either 100 or 0% are defined in a plane log t 1 /log b O ( b O is the adsorption coefficient); the diffusional or surface character…

General Chemical EngineeringDrop (liquid)Analytical chemistryVoltchemistry.chemical_elementDropping mercury electrodeAnalytical ChemistryMercury (element)SphericityAdsorptionchemistryElectrodeElectrochemistryOhmic contactJournal of Electroanalytical Chemistry
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"Table 15" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Sphericity distribution. Corrected to final state particles.

InclusiveE+ E- --> NEUTRAL XE+ E- ScatteringE+ E- --> CHARGED X91.2Single Differential DistributionDN/DSPHERICITY
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