Performance of JetMET high level trigger algorithms in the CMS experiment using proton-proton collisions data at sqrt(s) = 13 TeV during Run-2 (CMS DP-2022/063)
The performance of the high level trigger (HLT) algorithms involving jets and missing transverse momentum (MET or p
Tmiss) used in the CMS experiment are studied using full Run-2 luminosity of 137.5 fb−1. The analysed proton-proton collision dataset, having centre of mass energy 13
TeV, is recorded using orthogonal trigger algorithms, namely the isolated single muon or single electron triggers. The results are presented using trigger efficiency, defined as the fraction of collision events passing selections on HLT or online objects, plotted as a function of the transverse momenta (p
T) reconstructed offline. The efficiency vs. pileup is also shown in case of the p
Tmiss triggers.
More details can be found in the
DP-2022/063
note.
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The event selection efficiency for requiring the presence of at least one HLT PF jet having transverse momentum (pT) greater than 500 GeV, the lowest unprescaled threshold, is shown as a function of the pT of the offline PF jet in the event. The three different curves represent data collected in the years 2016, 2017 and 2018. The slight variation in turn-on is due to differences in offline jet energy scale calibrations. Get pdf version Contact: Pallabi Das |
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The event selection efficiency for requiring the HLT scalar energy sum (HT) greater than 900 GeV in 2016 and 1050 GeV in 2017, 2018, which correspond to the lowest unprescaled thresholds, is shown as a function of the offline HT. The 1050 GeV trigger is absent during 2016. The increased threshold in subsequent years is used to limit event acceptance with increasing pileup. The 2016 trigger efficiency also suffers from an effect due to Level-1 trigger seed firmware due to which the plateau does not reach 100%. Get pdf version Contact: Pallabi Das |
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The event selection efficiency for requiring the lowest unprescaled threshold HLT pTmiss triggers for the years 2016, 2017 and 2018 is shown as a function of the offline corrected pTmiss which takes into account jet energy scale corrections into the p Tmiss calculation. The online threshold was increased after 2016 to limit event acceptance due to pileup. Get pdf version Contact: Pallabi Das |
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The event selection efficiencies are compared by requiring the same threshold on nominal and corrected HLT pTmiss as a function of the offline corrected pTmiss in the year 2018. The HLT corrected pTmiss provides better turn-on at the expense of increased trigger rate. Get pdf version Contact: Pallabi Das |
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The event selection efficiencies are compared by requiring three different thresholds on nominal HLT pTmiss as a function of the offline corrected pTmiss in the year 2018. The trigger turn-on curves behave consistently. Get pdf version Contact: Pallabi Das |
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The event selection efficiencies as a function of pileup are compared between two thresholds determined using fixed efficiency values (80% and 95%) against the offline corrected pTmiss in the year 2016, referring to slide 6. The threshold at HLT applied on PF pTmiss is 170 GeV. Here we assume that the trigger efficiency plateau is reached at the chosen offline pTmiss threshold. It is observed that with increasing pileup the efficiency becomes worse. Get pdf version Contact: Pallabi Das |
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The event selection efficiencies as a function of pileup are compared between two thresholds determined using fixed efficiency values (80% and 95%) against the offline corrected pTmiss in the year 2017, referring to slide 6. The threshold at HLT applied on PF pTmiss is 250 GeV. Here we assume that the trigger efficiency plateau is reached at the chosen offline pTmiss threshold. It is observed that with increasing pileup the efficiency becomes worse. Get pdf version Contact: Pallabi Das |
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The event selection efficiencies as a function of pileup are compared between two thresholds determined using fixed efficiency values (80% and 95%) against the offline corrected pTmiss in the year 2018, referring to slide 6. The threshold at HLT applied on PF pTmiss is 200 GeV. Here we assume that the trigger efficiency plateau is reached at the chosen offline pTmiss threshold. It is observed that with increasing pileup the efficiency becomes worse. Get pdf version Contact: Pallabi Das |
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MilosDjordjevic - 2022-11-29