Search results for "Z(0)"

showing 10 items of 712 documents

"Table 73: Mass distribution, 2 tag, mbb window 420" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in th…

2018

The mass distribution of the llbb system used in the fit to derive the limits for the mbb window centered at 420 GeV for the nb = 2 (2 tag) category.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionmass distributionb-associated productionMHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 17" of "Measurements of $W^\pm Z$ production cross sections in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector and limits on ano…

2016

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Inclusive8000.0Proton-Proton ScatteringZ ProductionDifferential Cross SectionP P --> W- Z0 XAstrophysics::Cosmology and Extragalactic AstrophysicsTransverse Momentum DependenceW ProductionDSIG/DPTW
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"Table 13" of "Measurement of the production cross section for Z/gamma* in association with jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS d…

2014

Cross section for Inclusive Jet Multiplicity for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

Z ProductionHigh Energy Physics::PhenomenologyIntegrated Cross SectionAstrophysics::Instrumentation and Methods for AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsJet ProductionCross SectionSIGInclusiveP P --> Z0 JET XP P --> GAMMA* JET XProton-Proton ScatteringHigh Energy Physics::ExperimentComputer Science::Information Theory
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"Table 5" of "Measurements of $W^\pm Z$ production cross sections in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector and limits on anom…

2016

Cross section extrapolated to total phase space and all W and Z boson decays. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the theory uncertainty and the third is the luminosity uncertainty.

Inclusive8000.0Proton-Proton ScatteringZ ProductionAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross SectionP P --> (W+ + W-) Z0 XHigh Energy Physics::ExperimentAstrophysics::Cosmology and Extragalactic AstrophysicsCross SectionSIG
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"Table 4" of "Strange baryon production in Z hadronic decays"

1995

No description provided.

InclusiveE+ E- --> XIBAR+ XE+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringIntegrated Cross SectionE+ E- --> XI- XExclusive91.2Cross SectionR measurementSIG
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"Table 3" of "Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS…

2021

Signal selection acceptance times efficiency (A$\times \epsilon$), defined as the ratio of the number of MC signal events in the category to the number of generated signal events, as a function of the HVT resonance mass for the quark-antiquark production. The $A\times\epsilon$ is shown for each decay channel and the inclusive one. The decay of $W$ and $Z$ are to all flavors of leptons. The uncertainty shown represents the total statistical and systematic uncertainties.

WPRIME --> Z0 W13000.0resonanceHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologylvllHigh Energy Physics::ExperimentHVTWZW'
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"Table 6: Cross-section limits type-I tanb 10" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\el…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for an A boson in the type-I, tanbeta 10, 2HDM. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used. For type-I only gluon-gluon fusion is used and the nb=2 category only.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionCLScross section limitsHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 16" of "Properties of hadronic Z decays and test of QCD generators"

1992

Oblateness distribution.

DN/DOBLATENESSE+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringExclusive91.2Single Differential Distribution
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"Table 47: Mass distribution, 2 tag, mbb window 280" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in th…

2018

The mass distribution of the llbb system used in the fit to derive the limits for the mbb window centered at 280 GeV for the nb = 2 (2 tag) category.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionmass distributionb-associated productionMHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 6" of "Measurement of differential Z / gamma* + jet + X cross sections in p anti-p collisions at s**(1/2) = 1.96-TeV"

2008

Measurement of the cross section for inclusive Z0/GAMMA* production. The second DSYS error is from the muon identification and the third from the luminosity measurement.

InclusiveZ ProductionAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross SectionPBAR P --> GAMMA* XHigh Energy Physics::ExperimentJet ProductionPBAR P --> Z0 XCross SectionSIGMuon production
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