Search results for "NJET"

showing 10 items of 30 documents

"Table 20" of "Observation of electroweak $W^{\pm}Z$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} =$ 13 TeV wit…

2019

Measured $W^{pm}Zjj$ differential cross-section in the VBS fiducial phase space. The relative uncertainties are reported as percentages. The systematic uncertainties are in order of appearance: total uncorrelated systematic and correlated systematics related respectively to unfolding, electrons, muons, jets, reducible and irreducible backgrounds, pileup and luminosity. the last bin is a cross section for all events above the lower end of the bin.

13000.0Astrophysics::High Energy Astrophysical PhenomenaP P --> (W+ + W-) Z0 j j XDSIG/DNJETSGAP
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"Table 12" of "Observation of electroweak $W^{\pm}Z$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} =$ 13 TeV wit…

2019

Measured $W^{pm}Zjj$ differential cross-section in the VBS fiducial phase space. The relative uncertainties are reported as percentages. The systematic uncertainties are in order of appearance: total uncorrelated systematic and correlated systematics related respectively to unfolding, electrons, muons, jets, reducible and irreducible backgrounds, pileup and luminosity. The last bin is a cross section for all events above the lower end of the bin.

13000.0DSIG/DNJETSPT40Astrophysics::High Energy Astrophysical PhenomenaP P --> (W+ + W-) Z0 j j X
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"Table 13" of "Observation of electroweak $W^{\pm}Z$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} =$ 13 TeV wit…

2019

Correlation matrix for the unfolded fiducial cross-section.

13000.0DSIG/DNJETSPT40P P --> (W+ + W-) Z0 j j X
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"Table 21" of "Observation of electroweak $W^{\pm}Z$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} =$ 13 TeV wit…

2019

Correlation matrix for the unfolded fiducial cross-section.

13000.0P P --> (W+ + W-) Z0 j j XDSIG/DNJETSGAP
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Composite vignettes of Swedish male and female professional handball players’ career paths

2019

The aim of this study was to describe gender-specific career paths of Swedish professional handball players. A reanalysis of Ekengren et al. (2018) career interviews with nine male and nine female players led to creating two composite vignettes using the athletes’ own words, accounted for typical features in the male and female players’ career paths. Seven themes were identified in the analysis of the men’s transcripts and eight themes derived from the women’s transcripts. Further, the themes of both vignettes were aligned with career stages described in our previous study (Ekengren et al. 2018). The male players’ vignette is interpreted as a performance narrative congruent with elite handb…

Cultural StudiesbiologyAthletesGender relations05 social sciences030229 sport sciencesbiology.organism_classificationcultural praxis of athletes’ careerskäsipallourakehityssukupuoliDevelopmental psychology03 medical and health sciences0302 clinical medicinevinjetit0502 economics and businesscreative analytical practicePsychology050212 sport leisure & tourismurheilijatCareer developmentSport in Society
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"Table 41" 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 normalised 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 SectionDSIG/DNJETSP P --> (W+ + W-) Z0 XAstrophysics::Cosmology and Extragalactic Astrophysics
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"Table 27" 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 SectionDSIG/DNJETSP P --> (W+ + W-) Z0 XAstrophysics::Cosmology and Extragalactic Astrophysics
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"Table 26" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detec…

2013

The mean number of jets in the gap as a function of the mean transverse momentum of the boundary jets for boundary jets that have a rapidity difference in the range [1,2], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.

InclusiveDijet ProductionNJETProton-Proton ScatteringAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyP P --> JET JET X7000.0High Energy Physics::ExperimentJet Production
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"Table 29" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detec…

2013

The mean number of jets in the gap as a function of the mean transverse momentum of the boundary jets for boundary jets that have a rapidity difference in the range [4,5], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.

InclusiveDijet ProductionNJETProton-Proton ScatteringAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyP P --> JET JET X7000.0High Energy Physics::ExperimentJet Production
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"Table 28" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detec…

2013

The mean number of jets in the gap as a function of the mean transverse momentum of the boundary jets for boundary jets that have a rapidity difference in the range [3,4], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.

InclusiveDijet ProductionNJETProton-Proton ScatteringAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyP P --> JET JET X7000.0High Energy Physics::ExperimentJet Production
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