Performance of Etmiss triggers for heavy diboson searches in 2018 data ( CMS DP-2018/048)


TriggerTurnOn_SingleMu_met_pt_nomu_L_mu3_v4.png Efficiency plots for Single Muon Dataset versus ETmiss(no mu)
Trigger efficiencies for HLT_PFMETNoMu120_PFMHTNoMu120_IDTight trigger path, as a function of the offline ETmiss(no μ) variable, calculated in 2018 data. ETmiss(no μ) (at HLT/offline) is defined as the magnitude of the missing transverse momentum, reconstructed with the Particle Flow algorithm (at HLT/offline), removing the muon candidates from the vector sum. The missing hadronic activity HTmiss(no μ) is defined as the magnitude of the vector sum of the transverse momenta of the jets, reconstructed with the Particle Flow algorithm (at HLT level/offline), once the muon candidates have been removed.
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Contact: Lisa Benato

TriggerTurnOn_SingleMu_nPV_mu3nPV_v4.png Efficiency plots for Single Muon Dataset versus number of vertices
Trigger efficiencies for HLT_PFMETNoMu120_PFMHTNoMu120_IDTight trigger path, as a function of the number of primary vertices reconstructed offline, calculated in 2018 data. ETmiss(no μ) (at HLT level/offline) is defined as the magnitude of the missing transverse momentum, reconstructed with the Particle Flow algorithm (at HLT/offline), removing the muon candidates from the vector sum. The missing hadronic activity HTmiss(no μ) is defined as the magnitude of the vector sum of the transverse momenta of the jets, reconstructed with the Particle Flow algorithm (at HLT level/offline), once the muon candidates have been removed. Different offline thresholds of Emiss(no μ) are applied: 225 GeV (green); 275 GeV (orange); 325 GeV (light blue). A pile-up dependent inefficiency can be observed when the looser selection (green) is applied.
[Get pdf version]
Contact: Lisa Benato

-- ElisabettaGallo - 2018-07-13

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Topic revision: r1 - 2018-07-13 - ElisabettaGallo
 
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