Search results for "Ton-"

showing 10 items of 3657 documents

"Table 6" of "Observation of electroweak production of a same-sign $W$ boson pair in association with two jets in $pp$ collisions at $\sqrt{s}=13$ Te…

2019

Efficiency correction factor $C_{WW}$, defined as the ratio of the number of reconstructed $W^{\pm}W^{\pm}jj$ electroweak events in the signal region over the number of events generated in the fiducial phase space, in bins of the dilepton invariant mass, $m_{ll}$. The numbers are shown with their statistical and systematic uncertainties added in quadrature. The $C_{WW}$ factors have been calculated with Sherpa v2.2.2. The last bin includes the overflow.

Proton-Proton ScatteringW pair ProductionP P --> W- W- JET JETVBSP P --> W+ W+ JET JET13000Vector Boson Scattering
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"Table 4" of "Observation of electroweak production of a same-sign $W$ boson pair in association with two jets in $pp$ collisions at $\sqrt{s}=13$ Te…

2019

Impact of different components of systematic uncertainty on the measured fiducial cross section, without taking into account correlations. The impact of one source of systematic uncertainty is computed by first performing the fit with the corresponding nuisance parameter fixed to one standard deviation up or down from the value obtained in the nominal fit, then these up and down variations are symmetrized. The impacts of several sources of systematic uncertainty are added in quadrature for each component. The categorization of sources of systematic uncertainties into experimental and theory modeling correspond to those used for the measured fiducial cross section.

Proton-Proton ScatteringW pair ProductionP P --> W- W- JET JETVBSP P --> W+ W+ JET JET13000Vector Boson Scattering
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"Table 3" of "Observation of electroweak production of a same-sign $W$ boson pair in association with two jets in $pp$ collisions at $\sqrt{s}=13$ Te…

2019

The $m_{ll}$ distribution for events meeting all selection criteria for the signal region as predicted after the fit. The fitted signal strength and nuisance parameters have been propagated, with the exception of the uncertainties due to the interference and electroweak corrections for which a flat uncertainty is assigned. The last bin includes the overflow. The highest value measured in a candidate event in data is $m_{ll}=824$ GeV.

Proton-Proton ScatteringW pair ProductionP P --> W- W- JET JETVBSP P --> W+ W+ JET JET13000Vector Boson Scattering
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"Table 2" of "Observation of electroweak production of a same-sign $W$ boson pair in association with two jets in $pp$ collisions at $\sqrt{s}=13$ Te…

2019

The $m_{jj}$ distribution for events meeting all selection criteria for the signal region. Signal and individual background distributions are shown as predicted after the fit. The last bin includes the overflow. The highest value measured in a candidate event in data is $m_{jj}=3.8$ TeV.

Proton-Proton ScatteringW pair ProductionP P --> W- W- JET JETVBSP P --> W+ W+ JET JET13000Vector Boson Scattering
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"Table 24" of "Measurements of Wgamma and Zgamma production in pp collisions at sqrt{s}= 7 TeV with the ATLAS detector at the LHC"

2014

95% C.L. observed and expected upper limits on fiducial cross section of spin 1 narrow resonance decays to Zgamma (l+;l+;gamma) final state.

Proton-Proton ScatteringZ Production7000.0High Energy Physics::Experiment
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"Table 23" of "Measurements of Wgamma and Zgamma production in pp collisions at sqrt{s}= 7 TeV with the ATLAS detector at the LHC"

2014

The reconstruction efficiency of spin 1 narrow resonance rho_T in low scale technicolor model decays to Zgamma (l+;l-;gamma) final state with leading photon PT > 40 GeV.

Proton-Proton ScatteringZ ProductionAstrophysics::High Energy Astrophysical Phenomena7000.0High Energy Physics::Experiment
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"Table 17" of "Measurements of Wgamma and Zgamma production in pp collisions at sqrt{s}= 7 TeV with the ATLAS detector at the LHC"

2014

Normalised fiducial cross section of Zgamma (l+;l+;gamma) decay channel in bins of the jet multiplicity with leading photon pT > 15 GeV.

Proton-Proton ScatteringZ ProductionAstrophysics::High Energy Astrophysical Phenomena7000.0High Energy Physics::ExperimentAstrophysics::Cosmology and Extragalactic Astrophysics
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"Table 18" of "Measurements of Wgamma and Zgamma production in pp collisions at sqrt{s}= 7 TeV with the ATLAS detector at the LHC"

2014

Normalised fiducial cross section of Zgamma (l+;l+;gamma) decay channel in bins of the jet multiplicity with leading photon pT > 60 GeV.

Proton-Proton ScatteringZ ProductionAstrophysics::High Energy Astrophysical Phenomena7000.0High Energy Physics::ExperimentAstrophysics::Cosmology and Extragalactic Astrophysics
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"Table 20" of "Measurements of Wgamma and Zgamma production in pp collisions at sqrt{s}= 7 TeV with the ATLAS detector at the LHC"

2014

Normalised fiducial cross section of Zgamma (l+;l+;gamma) decay channel in bins of the mass of Zgamma with leading photon pT > 40 GeV.

Proton-Proton ScatteringZ ProductionAstrophysics::High Energy Astrophysical Phenomena7000.0High Energy Physics::ExperimentAstrophysics::Cosmology and Extragalactic Astrophysics
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"Table 5" of "Measurements of Wgamma and Zgamma production in pp collisions at sqrt{s}= 7 TeV with the ATLAS detector at the LHC"

2014

The measured inclusive fiducial cross section of Zgamma (nu;nubar;gamma) decay channel. The first systematic (sys) error is the combined systematic uncertainty excluding that of the luminosity. The second (sys) error is the uncertainty on the luminosity.

Proton-Proton ScatteringZ ProductionAstrophysics::High Energy Astrophysical Phenomena7000.0High Energy Physics::ExperimentAstrophysics::Cosmology and Extragalactic AstrophysicsNuclear Experiment
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