Search results for "W Pair Production"

showing 10 items of 30 documents

"Table 5" of "Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions…

2018

Inclusive Cross Section.

Photon-Photon ScatteringP P --> H --> WW (exclusive)8000.0W Pair ProductionProton-Proton ScatteringP P --> gamma gamma --> WWExclusiveCross SectionSIGDiffraction
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"Table 1" of "Search for new phenomena in the WW to l nu l' nu' final state in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector"

2012

Expected and observed 95% upper limits on cross section time branching ration for pp --> Graviton* < W+ W- >.

Proton-Proton ScatteringIntegrated Cross SectionW pair ProductionP P --> GRAVITONExclusive7000.0Cross SectionSIGW Production
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"Table 1" 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

Measured fiducial cross section.

Proton-Proton ScatteringIntegrated Cross SectionW pair ProductionP P --> W- W- JET JETVBSCross SectionSIGP P --> W+ W+ JET JET13000Vector Boson Scattering
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"Table 5" 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 dijet invariant mass, $m_{jj}$. 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 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 2" of "Measurement of the correlations between the polar angles of leptons from top quark decays in the helicity basis at $\sqrt{s}=7$TeV usin…

2017

The correlation factors for the statistical uncertainties between any two bins of the unfolded distribution.

Quantitative Biology::BiomoleculesP P --> LEPTON+ NU LEPTON- NUBAR BOTTOM BOTTOMBAR XDifferential Cross SectionP P --> W+ W- BOTTOM BOTTOMBAR XTopTop Production7000.0Astrophysics::Cosmology and Extragalactic AstrophysicsPhysics::Data Analysis; Statistics and ProbabilityP P --> TOP TOPBAR XInclusiveProton-Proton ScatteringW Pair ProductionAngular DependenceW ProductionDSIG/DTHETA
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"Table 1" of "Measurement of the correlations between the polar angles of leptons from top quark decays in the helicity basis at $\sqrt{s}=7$TeV usin…

2017

The numerical summary of the unfolded $\cos\theta_1\cdot\cos\theta_2$ distribution, with statistical and systematic uncertainties.

Quantitative Biology::BiomoleculesStatistics::TheoryP P --> LEPTON+ NU LEPTON- NUBAR BOTTOM BOTTOMBAR XDifferential Cross SectionMathematics::History and OverviewP P --> W+ W- BOTTOM BOTTOMBAR XTopTop Production7000.0P P --> TOP TOPBAR XInclusiveProton-Proton ScatteringW Pair ProductionAngular DependenceW ProductionDSIG/DTHETA
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