Search results for "data structure"

showing 10 items of 441 documents

"Table 66" 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 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 72" 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 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 74" 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 1MSVx 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 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 20" of "Search for a Heavy Neutral Particle Decaying to $e\mu$, $e\tau$, or $\mu\tau$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS De…

2015

Inputs used for the $\tilde{\nu}_{\tau}$-->$e\mu$ channel limit setting.

8000.0NComputer Science::Data Structures and AlgorithmsComputer Science::Information Theory
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"Table 43" of "Search for massive, long-lived particles using multitrack displaced vertices or displaced lepton pairs in pp collisions at $\sqrt{s}$ …

2015

Vertex mass distributions in data and one RPV SUSY signal model, for vertices with 0, 1 and $\geq$2 charged leptons in the dilepton $\mu^+\mu^-$ channel. The entries are the number of DVs in each bin, not normalized according to bin size. The signal model is for gluino pair production, with $\tilde{g}\to qq[\tilde{\chi}_1^0\to e\mu\nu/\mu\mu\nu]$ decays, $m(\tilde{g})$ = 1300 GeV, $m(\tilde{\chi}_1^0)$ = 50 GeV and $c\tau(\tilde{\chi}_1^0)$ = 30 mm.

8000.0Proton-Proton ScatteringHigh Energy Physics::PhenomenologyP P --> GLUINO GLUINOExclusiveHigh Energy Physics::ExperimentNComputer Science::Data Structures and Algorithms
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"Table 41" of "Search for massive, long-lived particles using multitrack displaced vertices or displaced lepton pairs in pp collisions at $\sqrt{s}$ …

2015

Vertex mass distributions in data and one RPV SUSY signal model, for vertices with 0, 1 and $\geq$2 charged leptons in the dilepton $e^+e^-$ channel. The entries are the number of DVs in each bin, not normalized according to bin size. The signal model is for gluino pair production, with $\tilde{g}\to qq[\tilde{\chi}_1^0\to e\mu\nu/ee\nu]$ decays, $m(\tilde{g})$ = 1300 GeV, $m(\tilde{\chi}_1^0)$ = 50 GeV and $c\tau(\tilde{\chi}_1^0)$ = 30 mm.

8000.0Proton-Proton ScatteringHigh Energy Physics::PhenomenologyP P --> GLUINO GLUINOExclusiveHigh Energy Physics::ExperimentNComputer Science::Data Structures and Algorithms
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