Search results for "LLP"

showing 10 items of 201 documents

"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 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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"Table 50" 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 $m_{s}=8$ GeV scalar benchmark sample for the combination of 1MSVx and 2MSVx strategies.

13000.0LLP$pp \rightarrow \varPhi \rightarrow ss$displaced hadronic jetsHigh Energy Physics::ExperimentScalar portalNuclear ExperimentSIG
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"Table 57" 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 $m_{s}=40$ 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 46" 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 $m_{s}=5$ 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 48" 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 $m_{s}=8$ 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 47" 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 $m_{s}=5$ GeV scalar benchmark sample for the combination of 1MSVx and 2MSVx strategies.

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