Search results for "dron"

showing 10 items of 4363 documents

"Table 75" 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 $\sigma \times B_{\tilde{g} \rightarrow \tilde{S} g}$ as a function of the proper lifetime $c\tau$ for $m_{\tilde{g}}=2000$ GeV for the combination of 1MSVx and 2MSVx strategies.

13000.0LLPdisplaced hadronic jetsStealth SUSYComputer Science::Data Structures and Algorithms$pp \rightarrow \tilde{g} (\rightarrow \tilde{S} g) \tilde{g} (\rightarrow \tilde{S} g)$SIG
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"Table 70" 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 $\sigma \times B_{\tilde{g} \rightarrow \tilde{S} g}$ as a function of the proper lifetime $c\tau$ for $m_{\tilde{g}}=1500$ GeV for 2MSVx strategy.

13000.0LLPdisplaced hadronic jetsStealth SUSYComputer Science::Data Structures and Algorithms$pp \rightarrow \tilde{g} (\rightarrow \tilde{S} g) \tilde{g} (\rightarrow \tilde{S} g)$SIG
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"Table 64" 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 $\sigma \times B_{\tilde{g} \rightarrow \tilde{S} g}$ as a function of the proper lifetime $c\tau$ for $m_{\tilde{g}}=800$ GeV for 2MSVx strategy.

13000.0LLPdisplaced hadronic jetsStealth SUSYComputer Science::Data Structures and Algorithms$pp \rightarrow \tilde{g} (\rightarrow \tilde{S} g) \tilde{g} (\rightarrow \tilde{S} g)$SIG
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"Table 63" 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 $\sigma \times B_{\tilde{g} \rightarrow \tilde{S} g}$ as a function of the proper lifetime $c\tau$ for $m_{\tilde{g}}=500$ GeV for the combination of 1MSVx and 2MSVx strategies.

13000.0LLPdisplaced hadronic jetsStealth SUSYComputer Science::Data Structures and Algorithms$pp \rightarrow \tilde{g} (\rightarrow \tilde{S} g) \tilde{g} (\rightarrow \tilde{S} g)$SIG
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"Table 9" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Moments of the Small Jet Broadening (BMIN) distributions at cm energies 133, 161, 172 and 183 GeV.

133.0-183.0Astrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringBMINExclusiveHigh Energy Physics::ExperimentJet ProductionNuclear Experiment
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"Table 11" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Moments of the Jet Broadening Difference (BDIFF) distributions at cm energies 133, 161, 172 and 183 GeV.

133.0-183.0Astrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringVARIANCENAME=BDIFFExclusiveHigh Energy Physics::ExperimentJet ProductionNuclear ExperimentBDIFF
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"Table 46" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

ALPHAS from the higher energies extrapolated to the Z0 mass. The second systematic (DSYS) error is the scale error.

133.0-183.0E+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringALPHASExclusiveJet Production
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"Table 5" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Moments of the Heavy Jet Mass (MH**2/EVIS**2) distributions at cm energies 133, 161, 172 and 183 GeV.

133.0-183.0E+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringMHEAVY-JET**2/EVIS**2ExclusiveVARIANCENAME=MHEAVY-JET**2/EVIS**2Jet ProductionSKEWNESSSNAME=MHEAVY-JET**2/EVIS**2
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"Table 1" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Moments of the (1-THRUST) distributions at cm energies 133, 161, 172 and 183 GeV.

133.0-183.0E+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringSKEWNESSNAME=THRUSTExclusiveVARIANCENAME=THRUSTTHRUSTJet Production
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"Table 7" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Moments of the Jet Mass Differences (MDIFF**2/EVIS**2) distributions at cm energies 133, 161, 172 and 183 GeV.

133.0-183.0E+ E- --> HADRONSE+ E- --> JETSMDIFF**2/EVIS**2E+ E- ScatteringExclusiveJet ProductionSKEWNESSNAME=MDIFF**2/EVIS**2VARIANCENAME=MDIFF**2/EVIS**2
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