Search results for "JETS"

showing 10 items of 1074 documents

"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 8" of "First measurement of the quark to photon fragmentation function"

1995

4-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).

E+ E- --> (JETS) 4JETFDSIG/SIGAstrophysics::High Energy Astrophysical PhenomenaE+ E- ScatteringIntegrated Cross SectionExclusiveHigh Energy Physics::ExperimentE+ E- --> GAMMA QUARK QUARKBAR90.912Jet ProductionCross SectionE+ E- --> (HADRONS) 2HADRON
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"Table 1" of "Determination of A(b)(FB) using jet charge measurements in Z decays."

1998

Only statistical errors are given for sqrt(s) = 89.43 and 92.97 GeV.

E+ E- --> BQ BQBARInclusiveAsymmetry MeasurementE+ E- --> Z0E+ E- ScatteringExclusiveHigh Energy Physics::ExperimentJet Production89.43-92.97Nuclear ExperimentE+ E- --> JETS XASYM
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"Table 45" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Three different schemes are used for evaluation of ALPHAS: (C=ALPHAS2) second alphas_s order, (C=NLLA) and (C=ALPHAS2+NLLA). See text of the paper for details. The second systematic (DSYS) error is the scale error.

E+ E- --> HADRONSE+ E- --> JETSE+ E- Scattering91.2-183.0ALPHASExclusiveJet Production
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"Table 15" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Distributions of Thrust Major (MAJOR) at cm energies 133, 161 and 172 GeV.

E+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringDN/DMAJORExclusiveSingle Differential DistributionJet Production133.0-172.0
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"Table 16" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Distribution of Thrust Major (MAJOR) at cm energy 183 GeV.

E+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringDN/DMAJORExclusiveSingle Differential DistributionJet Production183.0
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"Table 17" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Distributions of Thrust Minor (MINOR) at cm energies 133, 161 and 172 GeV.

E+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringDN/DMINORExclusiveSingle Differential DistributionJet Production133.0-172.0
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"Table 13" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Distributions of (1-THRUST) at cm energies 133, 161 and 172 GeV.

E+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringDN/DTHRUST}ExclusiveDN/DTHRUSTSingle Differential DistributionJet Production133.0-172.0
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