Search results for "Cross Section"

showing 10 items of 3111 documents

"Table 22" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XDSIG/DPTJet ProductionTransverse Momentum Dependence1960.0W Production
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"Table 24" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XDSIG/DPTJet ProductionTransverse Momentum Dependence1960.0W Production
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"Table 25" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XDSIG/DPTJet ProductionTransverse Momentum Dependence1960.0W Production
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"Table 11" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XHigh Energy Physics::ExperimentDSIG/DETARAPJet Production1960.0W Production
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"Table 9" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XHigh Energy Physics::ExperimentDSIG/DETARAPJet Production1960.0W Production
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"Table 12" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of lepton pseudorapidity for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XHigh Energy Physics::ExperimentDSIG/DETARAPJet Production1960.0W Production
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"Table 2" of "Study of $e^+e^- \rightarrow p\bar{p}$ in the vicinity of $\psi(3770)$"

2014

The two solutions of the dressed cross section and the corresponding phase angles, PHI.

Condensed Matter::Quantum GasesNonlinear Sciences::Exactly Solvable and Integrable SystemsE+ E- --> P PBARE+ E- Scattering3.65-3.9Integrated Cross SectionExclusivePsiPhysics::Atomic PhysicsCross SectionSIG
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"Table 134" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Oblateness distribution at c.m. energy 133.00 GeV.

Condensed Matter::Quantum GasesSingle Differential Cross Section133.0DSIG/DOBLATENESSE+ E- --> HADRONSE+ E- ScatteringPhysics::Space PhysicsPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentNuclear Experiment
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"Table 138" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Oblateness distribution at c.m. energy 189.00 GeV.

Condensed Matter::Quantum GasesSingle Differential Cross Section189.0DSIG/DOBLATENESSE+ E- --> HADRONSE+ E- ScatteringPhysics::Space PhysicsPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentNuclear Experiment
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"Table 140" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Oblateness distribution at c.m. energy 206.00 GeV.

Condensed Matter::Quantum GasesSingle Differential Cross SectionDSIG/DOBLATENESS206.0E+ E- --> HADRONSE+ E- ScatteringPhysics::Space PhysicsPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentNuclear Experiment
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