Search results for "Cross Section"

showing 10 items of 3111 documents

"Table 133" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Oblateness distribution at c.m. energy 91.20 GeV.

Condensed Matter::Quantum GasesSingle Differential Cross SectionDSIG/DOBLATENESSE+ E- --> HADRONSE+ E- ScatteringPhysics::Space PhysicsPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::Experiment91.2Nuclear Experiment
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"Table 135" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Oblateness distribution at c.m. energy 161.00 GeV.

Condensed Matter::Quantum GasesSingle Differential Cross SectionDSIG/DOBLATENESSE+ E- --> HADRONSE+ E- ScatteringPhysics::Space PhysicsPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentNuclear Experiment161.0
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"Table 136" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Oblateness distribution at c.m. energy 172.00 GeV.

Condensed Matter::Quantum GasesSingle Differential Cross SectionDSIG/DOBLATENESSE+ E- --> HADRONSE+ E- ScatteringPhysics::Space PhysicsPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentNuclear Experiment172.0
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"Table 137" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Oblateness distribution at c.m. energy 183.00 GeV.

Condensed Matter::Quantum GasesSingle Differential Cross SectionDSIG/DOBLATENESSE+ E- --> HADRONSE+ E- ScatteringPhysics::Space PhysicsPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentNuclear Experiment183.0
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"Table 139" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Oblateness distribution at c.m. energy 200.00 GeV.

Condensed Matter::Quantum GasesSingle Differential Cross SectionDSIG/DOBLATENESSE+ E- --> HADRONSE+ E- ScatteringPhysics::Space PhysicsPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentNuclear Experiment200.0
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"Table 1" of "A Precise Determination of the Number of Families With Light Neutrinos and of the $Z$ Boson Partial Widths"

1990

Penetrating charged particle track selection.

Condensed Matter::SuperconductivityE+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringIntegrated Cross Section88.278-95.036ExclusiveCross SectionR measurementSIG
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Effects of confinement level, cross-section shape and corner radius on the cyclic behavior of CFRCM confined concrete columns

2014

Abstract The main results of an experimental research aiming to investigate the behavior of medium-size low-strength concrete columns wrapped with Carbon Fiber Reinforced Cementitious Matrix (CFRCM) under monotonic and cyclic compressive axial loads are presented. Thirty columns with circular, square and rectangular cross-sections were tested under monotonic and cyclic axial loads to investigate the effect of the confinement level, the cross-section shape and the corner radius on the stiffness, strength, and ductility of CFRCM confined concrete columns under cyclic loads. The results prove that CFRCM confining jackets provide substantial gain in compressive strength, deformability and absor…

Corner radiusMaterials sciencebusiness.industryStiffnessBuilding and ConstructionStructural engineeringExperimental testsSquare (algebra)Cross section (physics)Settore ICAR/09 - Tecnica Delle CostruzioniCompressive strengthEnergy absorbingmedicineCementitious matrixGeneral Materials ScienceCarbon fiberComposite materialmedicine.symptomDuctilitybusinessCementitious matrixCyclic actionCivil and Structural EngineeringConfinement
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Limits on spin-dependent WIMP-nucleon cross sections from 225 live days of XENON100 data

2013

We present new experimental constraints on the elastic, spin-dependent WIMP-nucleon cross section using recent data from the XENON100 experiment, operated in the Laboratori Nazionali del Gran Sasso in Italy. An analysis of 224.6 live days x 34 kg of exposure acquired during 2011 and 2012 revealed no excess signal due to axial-vector WIMP interactions with 129-Xe and 131-Xe nuclei. This leads to the most stringent upper limits on WIMP-neutron cross sections for WIMP masses above 6 GeV, with a minimum cross section of 3.5 x 10^{-40} cm^2 at a WIMP mass of 45 GeV, at 90% confidence level.

Cosmology and Nongalactic Astrophysics (astro-ph.CO)[PHYS.ASTR.IM]Physics [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]Dark matterGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesdark matterParticle detectorHigh Energy Physics - ExperimentNuclear physicsCross section (physics)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)WIMP0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsPseudovectorInstrumentation and Methods for Astrophysics (astro-ph.IM)Spin-½Physics010308 nuclear & particles physics[SDU.ASTR.IM]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]High Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Astrophysics - Instrumentation and Methods for AstrophysicsNucleonAstrophysics - Cosmology and Nongalactic Astrophysics
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Production of a tensor glueball in the reaction γγ → G2π0 at large momentum transfer

2018

Abstract We study the production of a tensor glueball in the reaction γ γ → G 2 π 0 . We compute the cross section at higher momentum transfer using the collinear factorisation approach. We find that for a value of the tensor gluon coupling of f g T ∼ 100 MeV, the cross section can be measured in the near future by the Belle II experiment.

CouplingPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsGlueballMomentum transfer01 natural scienceslcsh:QC1-999GluonCross section (physics)Factorization0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)TensorNuclear Experiment010306 general physicslcsh:PhysicsPhysics Letters B
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A quantitative assessment of the effect of distributor type on particle circulation

1997

Abstract Garncarek's quantitative index of inhomogeneity has been used to compare the effect of distributor type on the degree of uniformity of solids mixing in a gas-fluidized bed assessed by following a tracer particle using the technique of Positron Emission Particle Tracking. The bed was a sand of 475 μm diameter fluidized at 2 U mf and contained within a column of 150 mm diameter. A porous and perforated plate distributor are compared. The index shows that tracer locations are generally more homogeneously distributed throughout the vertical section of the bed with the porous plate distributor. Behaviour varies with height and horizontal sections of the bed show that there is little dif…

Cross section (physics)ChemistryGeneral Chemical EngineeringBubbleMixing (process engineering)DistributorParticleMineralogyMechanicsFluidizationPorosityMagnetosphere particle motionPowder Technology
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