Search results for "Jet Production"

showing 10 items of 2071 documents

"Table 1" of "Measurement of the production cross section for W-bosons in association with jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS de…

2011

The measured cross section times branching ratio for W+jets in the electron channel as a function of corrected jet multiplicity.

Electron productionAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross Section7000.0Jet ProductionCross SectionP P --> W- JETS XSIGP P --> W+ JETS XInclusive2611940326119403Proton-Proton ScatteringHigh Energy Physics::ExperimentW Production
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"Table 3" of "Measurement of the production cross section for W-bosons in association with jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS de…

2011

The measured cross section ratio for W+jets in the electron channel as a function of corrected jet multiplicity.

Electron productionAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross Section7000.0Jet Productionrespiratory systemCross Sectionequipment and suppliesP P --> W- JETS XSIGcomplex mixturesP P --> W+ JETS XInclusive2611940326119403Proton-Proton ScatteringHigh Energy Physics::Experimenthuman activitiesW Productioncirculatory and respiratory physiologyComputer Science::Information Theory
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"Table 17" of "Search for supersymmetry in final states with jets, missing transverse momentum and one isolated lepton in sqrt{s} = 7 TeV pp collisio…

2016

Number of b-tagged jets in the combined electron plus three jets W+jets and top control region.

Electron productionAstrophysics::High Energy Astrophysical PhenomenaSUSY7000.0Jet ProductionP P --> E- .GE.3JET MM XNP P --> E+ .GE.3JET MM XInclusiveNonlinear Sciences::Exactly Solvable and Integrable SystemsProton-Proton ScatteringPhysics::Atomic and Molecular ClustersHigh Energy Physics::ExperimentSupersymmetry
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"Table 9" of "Measurement of the cross section for W-boson production in association with jets in ppbar collisions at s**(1/2) = 1.96-TeV"

2008

Total cross sections for W production in association with 4 or more jets.

Electron productionIntegrated Cross SectionJet Productionrespiratory systemCross Sectionequipment and suppliesSIGcomplex mixturesInclusivePBAR P --> W+ .GE.4JET XPBAR P --> W- .GE.4JET X1960.0human activitiesW Productioncirculatory and respiratory physiology
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"Table 6" of "Measurement of the cross section for W-boson production in association with jets in ppbar collisions at s**(1/2) = 1.96-TeV"

2008

Total cross sections for W production in association with 1 or more jets.

Electron productionIntegrated Cross SectionJet Productionrespiratory systemCross Sectionequipment and suppliesSIGcomplex mixturesInclusivePBAR P --> W- .GE.1JET X1960.0human activitiesPBAR P --> W+ .GE.1JET XW Productioncirculatory and respiratory physiology
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"Table 7" of "Measurement of the cross section for W-boson production in association with jets in ppbar collisions at s**(1/2) = 1.96-TeV"

2008

Total cross sections for W production in association with 2 or more jets.

Electron productionPBAR P --> W+ .GE.2JET XIntegrated Cross SectionPBAR P --> W- .GE.2JET XJet Productionrespiratory systemCross Sectionequipment and suppliesSIGcomplex mixturesInclusiveDijet Production1960.0human activitiesW Productioncirculatory and respiratory physiology
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"Table 3" of "First measurement of the quark to photon fragmentation function"

1995

2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).

FDSIG/SIGAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross SectionE+ E- --> GAMMA QUARK QUARKBARJet ProductionCross SectionE+ E- --> (HADRONS) 2HADRONDijet ProductionE+ E- ScatteringExclusiveHigh Energy Physics::Experiment90.912E+ E- --> 2JET
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"Table 4" of "First measurement of the quark to photon fragmentation function"

1995

2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).

FDSIG/SIGAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross SectionE+ E- --> GAMMA QUARK QUARKBARJet ProductionCross SectionE+ E- --> (HADRONS) 2HADRONDijet ProductionE+ E- ScatteringExclusiveHigh Energy Physics::Experiment90.912E+ E- --> 2JET
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"Table 1" of "First measurement of the quark to photon fragmentation function"

1995

2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).

FDSIG/SIGAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross SectionE+ E- --> GAMMA QUARK QUARKBARJet ProductionCross SectionE+ E- --> (HADRONS) 2HADRONDijet ProductionE+ E- ScatteringExclusiveHigh Energy Physics::Experiment90.912E+ E- --> 2JET
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"Table 2" of "First measurement of the quark to photon fragmentation function"

1995

2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).

FDSIG/SIGAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross SectionE+ E- --> GAMMA QUARK QUARKBARJet ProductionCross SectionE+ E- --> (HADRONS) 2HADRONDijet ProductionE+ E- ScatteringExclusiveHigh Energy Physics::Experiment90.912E+ E- --> 2JET
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