Search results for "Jets"

showing 10 items of 1074 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 92" of "Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS …

2018

Upper 95% CL limits on $\sigma\times B$ as a function of the proper lifetime $c\tau$ for $\chi \rightarrow \nu b \bar{b}$ channel with $m_{\chi}=30$ GeV ($m_{h}=125$ GeV) for 1MSVx strategy.

13000.0Higgs portal baryogenesisLLP$pp \rightarrow h \rightarrow \chi\chi$High Energy Physics::Phenomenologydisplaced hadronic jetsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 95" of "Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS …

2018

Upper 95% CL limits on $\sigma\times B$ as a function of the proper lifetime $c\tau$ for $\chi \rightarrow \nu b \bar{b}$ channel with $m_{\chi}=50$ GeV ($m_{h}=125$ GeV) for 1MSVx strategy.

13000.0Higgs portal baryogenesisLLP$pp \rightarrow h \rightarrow \chi\chi$High Energy Physics::Phenomenologydisplaced hadronic jetsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 97" of "Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS …

2018

Upper 95% CL limits on $\sigma\times B$ as a function of the proper lifetime $c\tau$ for $\chi \rightarrow \nu b \bar{b}$ channel with $m_{\chi}=100$ GeV ($m_{h}=125$ GeV) for 2MSVx strategy.

13000.0Higgs portal baryogenesisLLP$pp \rightarrow h \rightarrow \chi\chi$High Energy Physics::Phenomenologydisplaced hadronic jetsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 94" of "Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS …

2018

Upper 95% CL limits on $\sigma\times B$ as a function of the proper lifetime $c\tau$ for $\chi \rightarrow \nu b \bar{b}$ channel with $m_{\chi}=50$ GeV ($m_{h}=125$ GeV) for 2MSVx strategy.

13000.0Higgs portal baryogenesisLLP$pp \rightarrow h \rightarrow \chi\chi$High Energy Physics::Phenomenologydisplaced hadronic jetsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 91" of "Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS …

2018

Upper 95% CL limits on $\sigma\times B$ as a function of the proper lifetime $c\tau$ for $\chi \rightarrow \nu b \bar{b}$ channel with $m_{\chi}=30$ GeV ($m_{h}=125$ GeV) for 2MSVx strategy.

13000.0Higgs portal baryogenesisLLP$pp \rightarrow h \rightarrow \chi\chi$High Energy Physics::Phenomenologydisplaced hadronic jetsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 88" of "Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS …

2018

Upper 95% CL limits on $\sigma\times B$ as a function of the proper lifetime $c\tau$ for $\chi \rightarrow \nu b \bar{b}$ channel with $m_{\chi}=10$ GeV ($m_{h}=125$ GeV) for 2MSVx strategy.

13000.0Higgs portal baryogenesisLLP$pp \rightarrow h \rightarrow \chi\chi$High Energy Physics::Phenomenologydisplaced hadronic jetsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 89" of "Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS …

2018

Upper 95% CL limits on $\sigma\times B$ as a function of the proper lifetime $c\tau$ for $\chi \rightarrow \nu b \bar{b}$ channel with $m_{\chi}=10$ GeV ($m_{h}=125$ GeV) for 1MSVx strategy.

13000.0Higgs portal baryogenesisLLP$pp \rightarrow h \rightarrow \chi\chi$High Energy Physics::Phenomenologydisplaced hadronic jetsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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