Search results for "JETS"

showing 10 items of 1074 documents

"Table 8" of "Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS m…

2018

Barrel Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\chi \rightarrow \nu b \bar{b}$ benchmark samples ($m_{h}=125$ GeV). The trigger efficiency is defined as the fraction of LLPs selected by the Muon RoI Cluster trigger as a function of the LLP decay position. The trigger is efficient for hadronic decays of LLPs that occur anywhere from the outer regions of the HCal to the middle station of the MS. These efficiencies are obtained from the subset of events with only a single LLP decay in the muon spectrometer in order to ensure that the result of the trigger is due to a single burst of MS activity. The uncertainties shown are statistical only. The relative differences in ef…

13000.0Higgs portal baryogenesisLLPPhysics::Instrumentation and Detectors$pp \rightarrow h \rightarrow \chi\chi$displaced hadronic jetsHigh Energy Physics::ExperimentSIG
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"Table 21" 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

Endcap Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\chi \rightarrow lcb$ benchmark samples ($m_{h}=125$ GeV). The trigger efficiency is defined as the fraction of LLPs selected by the Muon RoI Cluster trigger as a function of the LLP decay position. The trigger is efficient for hadronic decays of LLPs that occur anywhere from the outer regions of the HCal to the middle station of the MS. These efficiencies are obtained from the subset of events with only a single LLP decay in the muon spectrometer in order to ensure that the result of the trigger is due to a single burst of MS activity. The uncertainties shown are statistical only. The relative differences in efficiencies…

13000.0Higgs portal baryogenesisLLPPhysics::Instrumentation and Detectors$pp \rightarrow h \rightarrow \chi\chi$displaced hadronic jetsHigh Energy Physics::ExperimentSIG
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"Table 7" of "Search for low-mass resonances decaying into two jets and produced in association with a photon using $pp$ collisions at $\sqrt{s} = 13…

2019

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the b-tagged category and masses below 450 GeV, for which the single-photon trigger was used.

13000.0High Energy Physics::Experimenttwo jets in association with a photonP P --> JET JET GAMMA XLow mass resonance search
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"Table 8" of "Search for low-mass resonances decaying into two jets and produced in association with a photon using $pp$ collisions at $\sqrt{s} = 13…

2019

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the b-tagged category and masses above 450 GeV, for which the combined trigger was used.

13000.0High Energy Physics::Experimenttwo jets in association with a photonP P --> JET JET GAMMA XLow mass resonance search
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"Table 5" of "Search for low-mass resonances decaying into two jets and produced in association with a photon using $pp$ collisions at $\sqrt{s} = 13…

2019

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the flavour-inclusive category and masses below 450 GeV, for which the single-photon trigger was used.

13000.0High Energy Physics::PhenomenologyHigh Energy Physics::Experimenttwo jets in association with a photonP P --> JET JET GAMMA XLow mass resonance search
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"Table 6" of "Search for low-mass resonances decaying into two jets and produced in association with a photon using $pp$ collisions at $\sqrt{s} = 13…

2019

Upper limits on Gaussian-shape contributions to the dijet mass distributions from the flavour-inclusive category and masses above 450 GeV, for which the combined trigger was used.

13000.0High Energy Physics::PhenomenologyHigh Energy Physics::Experimenttwo jets in association with a photonP P --> JET JET GAMMA XLow mass resonance search
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"Table 78" 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 $m_{\Phi}=200$ GeV and $m_{s}=8$ GeV scalar benchmark sample for 2MSVx strategy.

13000.0LLP$pp \rightarrow \varPhi \rightarrow ss$displaced hadronic jetsHigh Energy Physics::ExperimentScalar portalNuclear ExperimentSIG
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"Table 85" 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 $m_{\Phi}=1000$ GeV and $m_{s}=50$ GeV scalar benchmark sample for 2MSVx strategy.

13000.0LLP$pp \rightarrow \varPhi \rightarrow ss$displaced hadronic jetsHigh Energy Physics::ExperimentScalar portalNuclear ExperimentSIG
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"Table 52" 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 $\sigma/\sigma_{\textrm{SM}}\times B$ as a function of the proper lifetime $c\tau$ for $m_{\Phi}=125$ GeV and $m_{s}=15$ GeV scalar benchmark sample for 1MSVx strategy.

13000.0LLP$pp \rightarrow \varPhi \rightarrow ss$displaced hadronic jetsHigh Energy Physics::ExperimentScalar portalNuclear ExperimentSIG
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"Table 55" 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 $\sigma/\sigma_{\textrm{SM}}\times B$ as a function of the proper lifetime $c\tau$ for $m_{\Phi}=125$ GeV and $m_{s}=25$ GeV scalar benchmark sample for 1MSVx strategy.

13000.0LLP$pp \rightarrow \varPhi \rightarrow ss$displaced hadronic jetsHigh Energy Physics::ExperimentScalar portalNuclear ExperimentSIG
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