Search results for "dijet production"

showing 10 items of 348 documents

"Table 5" of "Investigation of the splitting of quark and gluon jets."

1998

Subjet multiplicity-1 as a function of the jet resolution parameter ycut for Quark jets in 'Y' topology events.

E+ E- --> HADRONS XHigh Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaE+ E- --> Z0High Energy Physics::Phenomenology91.2Jet ProductionMULTInclusiveDijet ProductionE+ E- --> 3JETE+ E- ScatteringExclusiveHigh Energy Physics::Experiment
researchProduct

"Table 6" of "Investigation of the splitting of quark and gluon jets."

1998

Subjet multiplicity-1 as a function of the jet resolution parameter ycut for Gluon jets in 'Y' topology events.

E+ E- --> HADRONS XInclusiveDijet ProductionE+ E- --> 3JETAstrophysics::High Energy Astrophysical PhenomenaE+ E- --> Z0E+ E- ScatteringHigh Energy Physics::PhenomenologyExclusiveHigh Energy Physics::Experiment91.2Jet ProductionMULT
researchProduct

"Table 13" of "Studies of quantum chromodynamics with the ALEPH detector"

1997

Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.

E+ E- --> HADRONSE+ E- --> Z0Integrated Cross Section91.2E+ E- --> 2JET XJet ProductionCross SectionSIGInclusiveDijet ProductionE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentR measurementComputer Science::Distributed Parallel and Cluster Computing
researchProduct

"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
researchProduct

"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
researchProduct

"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
researchProduct

"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
researchProduct

"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
researchProduct

"Table 16" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detec…

2013

The Gap Fraction as a function of the dijet veto energy, Q0, for boundary jets having a mean transverse momentum in the range [120,150} GeV and rapidity difference in the range [4,5]. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.

GAPFRACTIONInclusiveDijet ProductionProton-Proton ScatteringAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyP P --> JET JET X7000.0High Energy Physics::ExperimentJet Production
researchProduct

"Table 2" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detect…

2013

The Gap Fraction as a function of the mean transverse momentum of the boundary jets for boundary jets having a rapidity difference in the range [2,3], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.

GAPFRACTIONInclusiveDijet ProductionProton-Proton ScatteringAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyP P --> JET JET X7000.0High Energy Physics::ExperimentJet Production
researchProduct