Search results for "dijet"

showing 10 items of 417 documents

"Lund jet plane: horizontal slice, 1.52 < ln(1/z) < 1.80" of "Measurement of the Lund jet plane using charged particles in 13 TeV proton-proton…

2020

Normalized differential cross-section of the Lund jet plane. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties. The data is presented as a 1D distribution, for a single horizontal slice of the Lund jet plane between 1.52 < ln(1/z) < 1.80.

DijetsD^2SIG/DZDRProton-Proton ScatteringP P --> j jJet Substructure13000
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"Lund jet plane: horizontal slice, 2.36 < ln(1/z) < 2.63" of "Measurement of the Lund jet plane using charged particles in 13 TeV proton-proton…

2020

Normalized differential cross-section of the Lund jet plane. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties. The data is presented as a 1D distribution, for a single horizontal slice of the Lund jet plane between 2.36 < ln(1/z) < 2.63.

DijetsD^2SIG/DZDRProton-Proton ScatteringP P --> j jJet Substructure13000
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"Lund jet plane total covariance" of "Measurement of the Lund jet plane using charged particles in 13 TeV proton-proton collisions with the ATLAS det…

2020

The summed covariance matrix of all systematic and statistical uncertainties associated with the measurement in bins of $\ln{(1/z)} \times \ln{(R/\Delta R)}$.

DijetsD^2SIG/DZDRProton-Proton ScatteringP P --> j jJet Substructure13000
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"Lund jet plane: horizontal slice, 2.08 < ln(1/z) < 2.36" of "Measurement of the Lund jet plane using charged particles in 13 TeV proton-proton…

2020

Normalized differential cross-section of the Lund jet plane. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties. The data is presented as a 1D distribution, for a single horizontal slice of the Lund jet plane between 2.08 < ln(1/z) < 2.36.

DijetsD^2SIG/DZDRProton-Proton ScatteringP P --> j jJet Substructure13000
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"Lund jet plane: vertical slice, 0.67 < ln(R/#DeltaR) < 1.00" of "Measurement of the Lund jet plane using charged particles in 13 TeV proton-pr…

2020

Normalized differential cross-section of the Lund jet plane. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties. The data is presented as a 1D distribution, for a single vertical slice of the Lund jet plane between 0.67 < ln(R/#DeltaR) < 1.00.

DijetsD^2SIG/DZDRProton-Proton ScatteringP P --> j jJet Substructure13000
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"Lund jet plane: vertical slice, 4.00 < ln(R/#DeltaR) < 4.33" of "Measurement of the Lund jet plane using charged particles in 13 TeV proton-pr…

2020

Normalized differential cross-section of the Lund jet plane. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties. The data is presented as a 1D distribution, for a single vertical slice of the Lund jet plane between 4.00 < ln(R/#DeltaR) < 4.33.

DijetsProton-Proton ScatteringD^2SIG/DZDRJet SubstructureP P --> j j13000
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"Table 7" of "Investigation of the splitting of quark and gluon jets."

1998

Ratio of the sub-jet multiplicity-1 for gluon jets to the sub-jet multiplicity-1 for quark jets as a function of the jet resolution parameter ycut 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
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"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
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"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
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"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
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