Difference: HLTTauAllRun2 (1 vs. 2)

Revision 22019-06-19 - ElisabettaGallo

Line: 1 to 1
 
META TOPICPARENT name="HighLevelTriggerRunIIResults"

Tau Lepton Run 2 trigger Performance (CMS DP-2019/012)

Line: 8 to 8
 


Changed:
<
<
mutauEfficiencyPt_mediumTauMVA_2016DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert
>
>
mutauEfficiencyPt_mediumTauMVA_2016DataMC.png mu tauh trigger efficiency
The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline tau pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency.
Caption
[Get pdf version]
Contact: Hale Sert
 
Changed:
<
<
mutauEfficiencyPt_mediumTauMVA_2017DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert
>
>
mutauEfficiencyPt_mediumTauMVA_2017DataMC.png mu tauh trigger efficiency
The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline tau pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert
 
Changed:
<
<
mutauEfficiencyPt_mediumTauMVA_2018DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert
>
>
mutauEfficiencyPt_mediumTauMVA_2018DataMC.png mu tauh trigger efficiency
The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline tau pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency.
Caption
[Get pdf version]
Contact: Hale Sert
 


Changed:
<
<
mutauEfficiencyNvtx_mediumTauMVA_2016DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert
>
>
mutauEfficiencyNvtx_mediumTauMVA_2016DataMC.png mu tauh trigger efficiency
The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert
 
Changed:
<
<
mutauEfficiencyNvtx_mediumTauMVA_2017DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert
>
>
mutauEfficiencyNvtx_mediumTauMVA_2017DataMC.png mu tauh trigger efficiency
The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert
 
Changed:
<
<
mutauEfficiencyNvtx_mediumTauMVA_2018DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert
>
>
mutauEfficiencyNvtx_mediumTauMVA_2018DataMC.png mu tauh trigger efficiency
The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert
 
Added:
>
>

mutauEfficiencyEta_mediumTauMVA_2016DataMC.png mu tauh trigger efficiency
The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline tau eta for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert


mutauEfficiencyEta_mediumTauMVA_2017DataMC.png mu tauh trigger efficiency
The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline tau eta for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert


mutauEfficiencyEta_mediumTauMVA_2018DataMC.png mu tauh trigger efficiency
The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline tau eta for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert




etauEfficiencyPt_mediumTauMVA_2017DataMC.png e tauh trigger efficiency
The hadronic tau leg efficiencies of e-tau triggers are shown below as a function of offline tau pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert


etauEfficiencyPt_mediumTauMVA_2018DataMC.png e tauh trigger efficiency
The hadronic tau leg efficiencies of e-tau triggers are shown below as a function of offline tau pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency.
Caption
[Get pdf version]
Contact: Hale Sert


etauEfficiencyNvtx_mediumTauMVA_2017DataMC.png e tauh trigger efficiency
The hadronic tau leg efficiencies of e-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 35 GeV for both 2017 and 2018. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert


etauEfficiencyNvtx_mediumTauMVA_2018DataMC.png e tauh trigger efficiency
The hadronic tau leg efficiencies of e-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 35 GeV for both 2017 and 2018.
Caption
[Get pdf version]
Contact: Hale Sert


etauEfficiencyEta_mediumTauMVA_2017DataMC.png e tauh trigger efficiency
The hadronic tau leg efficiencies of e-tau triggers are shown below as a function of offline tau eta for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 35 GeV for both 2017 and 2018. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert


etauEfficiencyEta_mediumTauMVA_2018DataMC.png e tauh trigger efficiency
The hadronic tau leg efficiencies of e-tau triggers are shown below as a function of offline tau eta for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 35 GeV for both 2017 and 2018.
Caption
[Get pdf version]
Contact: Hale Sert



ditauEfficiencyPt_mediumTauMVA_2016DataMC.png di-tauh trigger efficiency
The hadronic tau leg efficiencies of di-tau triggers are shown below as a function of offline tau pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency.
Caption
[Get pdf version]
Contact: Hale Sert


ditauEfficiencyPt_mediumTauMVA_2017DataMC.png di-tauh trigger efficiency
The hadronic tau leg efficiencies of di-tau triggers are shown below as a function of offline tau pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert


ditauEfficiencyPt_mediumTauMVA_2018DataMC.png di-tauh trigger efficiency
The hadronic tau leg efficiencies of di-tau triggers are shown below as a function of offline tau pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency.
Caption
[Get pdf version]
Contact: Hale Sert


ditauEfficiencyNvtx_mediumTauMVA_2016DataMC.png di-tauh trigger efficiency
The hadronic tau leg efficiencies of di-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 50 GeV for every year.
Caption
[Get pdf version]
Contact: Hale Sert


ditauEfficiencyNvtx_mediumTauMVA_2017DataMC.png di-tauh trigger efficiency
The hadronic tau leg efficiencies of di-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 50 GeV for every year. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert


ditauEfficiencyNvtx_mediumTauMVA_2018DataMC.png di-tauh trigger efficiency
The hadronic tau leg efficiencies of di-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 50 GeV for every year.
Caption
[Get pdf version]
Contact: Hale Sert


ditauEfficiencyEta_mediumTauMVA_2016DataMC.png di-tauh trigger efficiency
The hadronic tau leg efficiencies of di-tau triggers are shown below as a function of offline tau eta for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 50 GeV for every year.
Caption
[Get pdf version]
Contact: Hale Sert


ditauEfficiencyEta_mediumTauMVA_2017DataMC.png di-tauh trigger efficiency
The hadronic tau leg efficiencies of di-tau triggers are shown below as a function of offline tau eta for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 50 GeV for every year. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert


ditauEfficiencyEta_mediumTauMVA_2018DataMC.png di-tauh trigger efficiency
The hadronic tau leg efficiencies of di-tau triggers are shown below as a function of offline tau eta for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pT is applied to be above the trigger threshold: pT > 50 GeV for every year.
Caption
[Get pdf version]
Contact: Hale Sert



mutauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.png HPS based and Cone based tau reconstruction comparison
HPS tau reconstruction was deployed at HLT in the beginning of 2018 data-taking. The efficiency of hadronic tau leg of the mu-tau trigger is shown as a function of offline tau pT for the 17.7 fb-1 data taken with the cone-based tau reconstruction and for 42.0 fb-1 data collected with the HPS-based algorithm in 2018. The combined L1 and HLT efficiency of the tau<sub<h-leg is shown. The HPS-based tauh reconstruction algorithm has a rate of 4.6 Hz for mu-tau and 39 Hz for di-tau triggers at = 50, while the rates for cone-based algorithm was 5.2 for mu-tau and 50 Hz for di-tau triggers. So, the HPS reduces the rates by 10% and 20% for mu-tau and di-tau triggers, respectively [Ref: CMS DP -2018/035].
Caption
[Get pdf version]
Contact: Hale Sert

ditauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.png HPS based and Cone based tau reconstruction comparison
HPS tau reconstruction was deployed at HLT in the beginning of 2018 data-taking. The efficiency of hadronic tau leg of the di-tau trigger is shown as a function of offline tau pT for the 17.7 fb-1 data taken with the cone-based tau reconstruction and for 42.0 fb-1 data collected with the HPS-based algorithm in 2018. The combined L1 and HLT efficiency of the tau<sub<h-leg is shown. The HPS-based tauh reconstruction algorithm has a rate of 4.6 Hz for mu-tau and 39 Hz for di-tau triggers at = 50, while the rates for cone-based algorithm was 5.2 for mu-tau and 50 Hz for di-tau triggers. So, the HPS reduces the rates by 10% and 20% for mu-tau and di-tau triggers, respectively [Ref: CMS DP-2018/035].
Caption
[Get pdf version]
Contact: Hale Sert

mutauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.png HPS based and Cone based tau reconstruction comparison
HPS tau reconstruction was deployed at HLT in the beginning of 2018 data-taking. The efficiency of hadronic tau leg of the mu-tau trigger is shown as a function of number of vertices for the 17.7 fb-1 data taken with the cone-based tau reconstruction and for 42.0 fb-1 data collected with the HPS-based algorithm in 2018. The combined L1 and HLT efficiency of the tau<sub<h-leg is shown. The HPS-based tauh reconstruction algorithm has a rate of 4.6 Hz for mu-tau and 39 Hz for di-tau triggers at = 50, while the rates for cone-based algorithm was 5.2 for mu-tau and 50 Hz for di-tau triggers. So, the HPS reduces the rates by 10% and 20% for mu-tau and di-tau triggers, respectively [Ref: CMS DP-2018/035].
Caption
[Get pdf version]
Contact: Hale Sert

ditauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.png HPS based and Cone based tau reconstruction comparison
HPS tau reconstruction was deployed at HLT in the beginning of 2018 data-taking. The efficiency of hadronic tau leg of the di-tau trigger is shown as a function of number of vertices for the 17.7 fb-1 data taken with the cone-based tau reconstruction and for 42.0 fb-1 data collected with the HPS-based algorithm in 2018. The combined L1 and HLT efficiency of the tau<sub<h-leg is shown. The HPS-based tauh reconstruction algorithm has a rate of 4.6 Hz for mu-tau and 39 Hz for di-tau triggers at = 50, while the rates for cone-based algorithm was 5.2 for mu-tau and 50 Hz for di-tau triggers. So, the HPS reduces the rates by 10% and 20% for mu-tau and di-tau triggers, respectively [Ref: CMS DP-2018/035].
Caption
[Get pdf version]
Contact: Hale Sert



ptResolution_mutau_2018ABCD_HPSBeforeAfter.png pT resolution of HPS-based and cone-based tau reconstruction
pT resolution of the HPS based and cone-based tau reconstruction is shown on the right. The resolution is calculated for mu-tauh trigger by comparing pT of the online and offline tau leptons. It is calculated using the first 17.7 fb-1 of data taken with the cone-based tau reconstruction, where the trigger paths with HPS based algorithm was included for the purpose of testing. The HPS-based tauh reconstruction has better pT resolution compared to the cone-based reconstruction.
Caption
[Get pdf version]
Contact: Hale Sert



mutauEfficiencyPt_eachYear_mediumTauMVA_Data.png Performance of triggers in Run 2
The hadronic tau leg efficiencies of mu-tauhtriggers are shown below as a function of offline tau pT for 2016, 2017 and 2018 years overlaid with each other. The shown efficiencies correspond to the combined L1 and HLT efficiency. The different HLT thresholds and differences on L1 seed result in higher efficiencies in 2016 and differences in shapes of the 2016 efficiencies in mu-tau and e-tau triggers compared to 2017 and 2018. The low pileup in 2016 has also an impact for the higher efficiencies in each trigger
Caption
[Get pdf version]
Contact: Hale Sert

etauEfficiencyPt_eachYear_mediumTauMVA_Data.png Performance of triggers in Run 2
The hadronic tau leg efficiencies of e-tauhtriggers are shown below as a function of offline tau pT for 2016, 2017 and 2018 years overlaid with each other. The shown efficiencies correspond to the combined L1 and HLT efficiency. The different HLT thresholds and differences on L1 seed result in higher efficiencies in 2016 and differences in shapes of the 2016 efficiencies in mu-tau and e-tau triggers compared to 2017 and 2018. The low pileup in 2016 has also an impact for the higher efficiencies in each trigger
Caption
[Get pdf version]
Contact: Hale Sert

ditauEfficiencyPt_eachYear_mediumTauMVA_Data.png Performance of triggers in Run 2
The hadronic tau leg efficiencies of di-tauhtriggers are shown below as a function of offline tau pT for 2016, 2017 and 2018 years overlaid with each other. The shown efficiencies correspond to the combined L1 and HLT efficiency. The different HLT thresholds and differences on L1 seed result in higher efficiencies in 2016 and differences in shapes of the 2016 efficiencies in mu-tau and e-tau triggers compared to 2017 and 2018. The low pileup in 2016 has also an impact for the higher efficiencies in each trigger
Caption
[Get pdf version]
Contact: Hale Sert

mutauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png Performance of triggers in Run 2
The hadronic tau leg efficiencies of mu-tauhtriggers are shown below as a function of number of vertices for 2016, 2017 and 2018 years overlaid with each other. The shown efficiencies correspond to the combined L1 and HLT efficiency. In these plots an offline cut on the tau pT is applied to be above the trigger thresholds. The corresponding cuts are represented on the legends. The low pileup in 2016 has also an impact for the higher efficiencies in each trigger
Caption
[Get pdf version]
Contact: Hale Sert

etauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png Performance of triggers in Run 2
The hadronic tau leg efficiencies of e-tauhtriggers are shown below as a function of number of vertices for 2016, 2017 and 2018 years overlaid with each other. The shown efficiencies correspond to the combined L1 and HLT efficiency. In these plots an offline cut on the tau pT is applied to be above the trigger thresholds. The corresponding cuts are represented on the legends. The low pileup in 2016 has also an impact for the higher efficiencies in each trigger
Caption
[Get pdf version]
Contact: Hale Sert

ditauEfficiencyNtvx_eachYear_mediumTauMVA_Data.png Performance of triggers in Run 2
The hadronic tau leg efficiencies of di-tauhtriggers are shown below as a function of number of vertices for 2016, 2017 and 2018 years overlaid with each other. The shown efficiencies correspond to the combined L1 and HLT efficiency. In these plots an offline cut on the tau pT is applied to be above the trigger thresholds. The corresponding cuts are represented on the legends. The low pileup in 2016 has also an impact for the higher efficiencies in each trigger
Caption
[Get pdf version]
Contact: Hale Sert
 

-- ElisabettaGallo - 2019-06-18

Line: 78 to 167
 
META FILEATTACHMENT attachment="etauEfficiencyPt_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560848209" name="etauEfficiencyPt_mediumTauMVA_2018DataMC.png" path="etauEfficiencyPt_mediumTauMVA_2018DataMC.png" size="20714" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560848209" name="mutauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" path="mutauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" size="16021" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyEta_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560848209" name="mutauEfficiencyEta_mediumTauMVA_2018DataMC.png" path="mutauEfficiencyEta_mediumTauMVA_2018DataMC.png" size="19726" user="egallo" version="1"
Added:
>
>
META FILEATTACHMENT attachment="ditauEfficiencyEta_mediumTauMVA_2016DataMC.pdf" attr="" comment="" date="1560938176" name="ditauEfficiencyEta_mediumTauMVA_2016DataMC.pdf" path="ditauEfficiencyEta_mediumTauMVA_2016DataMC.pdf" size="16014" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyEta_mediumTauMVA_2016DataMC.png" attr="" comment="" date="1560938176" name="ditauEfficiencyEta_mediumTauMVA_2016DataMC.png" path="ditauEfficiencyEta_mediumTauMVA_2016DataMC.png" size="20345" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyEta_mediumTauMVA_2017DataMC.pdf" attr="" comment="" date="1560938176" name="ditauEfficiencyEta_mediumTauMVA_2017DataMC.pdf" path="ditauEfficiencyEta_mediumTauMVA_2017DataMC.pdf" size="16002" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyEta_mediumTauMVA_2017DataMC.png" attr="" comment="" date="1560938176" name="ditauEfficiencyEta_mediumTauMVA_2017DataMC.png" path="ditauEfficiencyEta_mediumTauMVA_2017DataMC.png" size="20710" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560938176" name="ditauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" path="ditauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" size="15996" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyEta_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560938176" name="ditauEfficiencyEta_mediumTauMVA_2018DataMC.png" path="ditauEfficiencyEta_mediumTauMVA_2018DataMC.png" size="20467" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyNvtx_mediumTauMVA_2016DataMC.pdf" attr="" comment="" date="1560938244" name="ditauEfficiencyNvtx_mediumTauMVA_2016DataMC.pdf" path="ditauEfficiencyNvtx_mediumTauMVA_2016DataMC.pdf" size="14539" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyNvtx_mediumTauMVA_2016DataMC.png" attr="" comment="" date="1560938244" name="ditauEfficiencyNvtx_mediumTauMVA_2016DataMC.png" path="ditauEfficiencyNvtx_mediumTauMVA_2016DataMC.png" size="20321" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyNvtx_mediumTauMVA_2017DataMC.pdf" attr="" comment="" date="1560938244" name="ditauEfficiencyNvtx_mediumTauMVA_2017DataMC.pdf" path="ditauEfficiencyNvtx_mediumTauMVA_2017DataMC.pdf" size="14660" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyNvtx_mediumTauMVA_2017DataMC.png" attr="" comment="" date="1560938244" name="ditauEfficiencyNvtx_mediumTauMVA_2017DataMC.png" path="ditauEfficiencyNvtx_mediumTauMVA_2017DataMC.png" size="20454" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyNvtx_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560938244" name="ditauEfficiencyNvtx_mediumTauMVA_2018DataMC.pdf" path="ditauEfficiencyNvtx_mediumTauMVA_2018DataMC.pdf" size="14656" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyNvtx_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560938244" name="ditauEfficiencyNvtx_mediumTauMVA_2018DataMC.png" path="ditauEfficiencyNvtx_mediumTauMVA_2018DataMC.png" size="20294" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_mediumTauMVA_2016DataMC.pdf" attr="" comment="" date="1560938283" name="ditauEfficiencyPt_mediumTauMVA_2016DataMC.pdf" path="ditauEfficiencyPt_mediumTauMVA_2016DataMC.pdf" size="14990" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_mediumTauMVA_2016DataMC.png" attr="" comment="" date="1560938283" name="ditauEfficiencyPt_mediumTauMVA_2016DataMC.png" path="ditauEfficiencyPt_mediumTauMVA_2016DataMC.png" size="20668" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyNvtx_eachYear_mediumTauMVA_Data.pdf" attr="" comment="" date="1560940703" name="ditauEfficiencyNvtx_eachYear_mediumTauMVA_Data.pdf" path="ditauEfficiencyNvtx_eachYear_mediumTauMVA_Data.pdf" size="15012" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png" attr="" comment="" date="1560940703" name="ditauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png" path="ditauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png" size="22576" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_eachYear_mediumTauMVA_Data.pdf" attr="" comment="" date="1560938662" name="mutauEfficiencyNvtx_eachYear_mediumTauMVA_Data.pdf" path="mutauEfficiencyNvtx_eachYear_mediumTauMVA_Data.pdf" size="15058" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png" attr="" comment="" date="1560938662" name="mutauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png" path="mutauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png" size="21859" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_eachYear_mediumTauMVA_Data.pdf" attr="" comment="" date="1560940740" name="ditauEfficiencyPt_eachYear_mediumTauMVA_Data.pdf" path="ditauEfficiencyPt_eachYear_mediumTauMVA_Data.pdf" size="15712" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_eachYear_mediumTauMVA_Data.png" attr="" comment="" date="1560940740" name="ditauEfficiencyPt_eachYear_mediumTauMVA_Data.png" path="ditauEfficiencyPt_eachYear_mediumTauMVA_Data.png" size="23280" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_eachYear_mediumTauMVA_Data.pdf" attr="" comment="" date="1560940790" name="mutauEfficiencyPt_eachYear_mediumTauMVA_Data.pdf" path="mutauEfficiencyPt_eachYear_mediumTauMVA_Data.pdf" size="15751" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_eachYear_mediumTauMVA_Data.png" attr="" comment="" date="1560940790" name="mutauEfficiencyPt_eachYear_mediumTauMVA_Data.png" path="mutauEfficiencyPt_eachYear_mediumTauMVA_Data.png" size="22835" user="egallo" version="1"

Revision 12019-06-18 - ElisabettaGallo

Line: 1 to 1
Added:
>
>
META TOPICPARENT name="HighLevelTriggerRunIIResults"

Tau Lepton Run 2 trigger Performance (CMS DP-2019/012)

The trigger efficiency is estimated using Tag and Probe (TnP) method in Z -> tautau -> mu tauh events. Details about the procedure can be found in the DP note.


mutauEfficiencyPt_mediumTauMVA_2016DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert


mutauEfficiencyPt_mediumTauMVA_2017DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert


mutauEfficiencyPt_mediumTauMVA_2018DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of offline pt for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert


mutauEfficiencyNvtx_mediumTauMVA_2016DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert


mutauEfficiencyNvtx_mediumTauMVA_2017DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively. The encountered pixel problems in 2017 cause a reduced efficiency compared to simulation.
Caption
[Get pdf version]
Contact: Hale Sert


mutauEfficiencyNvtx_mediumTauMVA_2018DataMC.png mu tauh trigger efficiency The hadronic tau leg efficiencies of mu-tau triggers are shown below as a function of number of vertices for each year. The shown efficiencies correspond to the combined L1 and HLT efficiency. An offline cut on the tau pt is applied to be above the trigger threshold, > 35, 42, 42 GeV for 2016, 2017, 2018, respectively.
Caption
[Get pdf version]
Contact: Hale Sert

-- ElisabettaGallo - 2019-06-18

META FILEATTACHMENT attachment="ditauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.pdf" attr="" comment="" date="1560847932" name="ditauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.pdf" path="ditauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.pdf" size="14612" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.png" attr="" comment="" date="1560847932" name="ditauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.png" path="ditauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.png" size="17026" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.pdf" attr="" comment="" date="1560847932" name="ditauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.pdf" path="ditauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.pdf" size="15308" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.png" attr="" comment="" date="1560847932" name="ditauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.png" path="ditauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.png" size="17164" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.png" attr="" comment="" date="1560847932" name="mutauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.png" path="mutauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.png" size="16786" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.pdf" attr="" comment="" date="1560847932" name="mutauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.pdf" path="mutauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.pdf" size="15302" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.png" attr="" comment="" date="1560847932" name="mutauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.png" path="mutauEfficiencyPt_mediumTauMVA_2018_ConeVSHPS.png" size="17076" user="egallo" version="1"
META FILEATTACHMENT attachment="ptResolution_mutau_2018ABCD_HPSBeforeAfter.pdf" attr="" comment="" date="1560847932" name="ptResolution_mutau_2018ABCD_HPSBeforeAfter.pdf" path="ptResolution_mutau_2018ABCD_HPSBeforeAfter.pdf" size="17178" user="egallo" version="1"
META FILEATTACHMENT attachment="ptResolution_mutau_2018ABCD_HPSBeforeAfter.png" attr="" comment="" date="1560847932" name="ptResolution_mutau_2018ABCD_HPSBeforeAfter.png" path="ptResolution_mutau_2018ABCD_HPSBeforeAfter.png" size="16322" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.pdf" attr="" comment="" date="1560847932" name="mutauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.pdf" path="mutauEfficiencyNvtx_mediumTauMVA_2018_ConeVSHPS.pdf" size="14588" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyEta_mediumTauMVA_2017DataMC.pdf" attr="" comment="" date="1560848004" name="etauEfficiencyEta_mediumTauMVA_2017DataMC.pdf" path="etauEfficiencyEta_mediumTauMVA_2017DataMC.pdf" size="16026" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyEta_mediumTauMVA_2017DataMC.png" attr="" comment="" date="1560848004" name="etauEfficiencyEta_mediumTauMVA_2017DataMC.png" path="etauEfficiencyEta_mediumTauMVA_2017DataMC.png" size="20744" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560848004" name="etauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" path="etauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" size="16027" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyEta_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560848004" name="etauEfficiencyEta_mediumTauMVA_2018DataMC.png" path="etauEfficiencyEta_mediumTauMVA_2018DataMC.png" size="20521" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyNvtx_eachYear_mediumTauMVA_Data.pdf" attr="" comment="" date="1560848004" name="etauEfficiencyNvtx_eachYear_mediumTauMVA_Data.pdf" path="etauEfficiencyNvtx_eachYear_mediumTauMVA_Data.pdf" size="15191" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png" attr="" comment="" date="1560848004" name="etauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png" path="etauEfficiencyNvtx_eachYear_mediumTauMVA_Data.png" size="26319" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyNvtx_mediumTauMVA_2017DataMC.pdf" attr="" comment="" date="1560848004" name="etauEfficiencyNvtx_mediumTauMVA_2017DataMC.pdf" path="etauEfficiencyNvtx_mediumTauMVA_2017DataMC.pdf" size="14676" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyNvtx_mediumTauMVA_2017DataMC.png" attr="" comment="" date="1560848004" name="etauEfficiencyNvtx_mediumTauMVA_2017DataMC.png" path="etauEfficiencyNvtx_mediumTauMVA_2017DataMC.png" size="20612" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyNvtx_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560848004" name="etauEfficiencyNvtx_mediumTauMVA_2018DataMC.pdf" path="etauEfficiencyNvtx_mediumTauMVA_2018DataMC.pdf" size="14651" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyNvtx_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560848004" name="etauEfficiencyNvtx_mediumTauMVA_2018DataMC.png" path="etauEfficiencyNvtx_mediumTauMVA_2018DataMC.png" size="20460" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_mediumTauMVA_2017DataMC.pdf" attr="" comment="" date="1560848094" name="mutauEfficiencyNvtx_mediumTauMVA_2017DataMC.pdf" path="mutauEfficiencyNvtx_mediumTauMVA_2017DataMC.pdf" size="14681" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_mediumTauMVA_2017DataMC.png" attr="" comment="" date="1560848094" name="mutauEfficiencyNvtx_mediumTauMVA_2017DataMC.png" path="mutauEfficiencyNvtx_mediumTauMVA_2017DataMC.png" size="19793" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560848094" name="mutauEfficiencyNvtx_mediumTauMVA_2018DataMC.pdf" path="mutauEfficiencyNvtx_mediumTauMVA_2018DataMC.pdf" size="14668" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560848094" name="mutauEfficiencyNvtx_mediumTauMVA_2018DataMC.png" path="mutauEfficiencyNvtx_mediumTauMVA_2018DataMC.png" size="19685" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_mediumTauMVA_2016DataMC.pdf" attr="" comment="" date="1560848094" name="mutauEfficiencyPt_mediumTauMVA_2016DataMC.pdf" path="mutauEfficiencyPt_mediumTauMVA_2016DataMC.pdf" size="14951" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_mediumTauMVA_2016DataMC.png" attr="" comment="" date="1560848094" name="mutauEfficiencyPt_mediumTauMVA_2016DataMC.png" path="mutauEfficiencyPt_mediumTauMVA_2016DataMC.png" size="20154" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_mediumTauMVA_2017DataMC.pdf" attr="" comment="" date="1560848094" name="mutauEfficiencyPt_mediumTauMVA_2017DataMC.pdf" path="mutauEfficiencyPt_mediumTauMVA_2017DataMC.pdf" size="14999" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_mediumTauMVA_2017DataMC.png" attr="" comment="" date="1560848094" name="mutauEfficiencyPt_mediumTauMVA_2017DataMC.png" path="mutauEfficiencyPt_mediumTauMVA_2017DataMC.png" size="20087" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560848094" name="mutauEfficiencyPt_mediumTauMVA_2018DataMC.pdf" path="mutauEfficiencyPt_mediumTauMVA_2018DataMC.pdf" size="15000" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyPt_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560848094" name="mutauEfficiencyPt_mediumTauMVA_2018DataMC.png" path="mutauEfficiencyPt_mediumTauMVA_2018DataMC.png" size="20101" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_mediumTauMVA_2017DataMC.pdf" attr="" comment="" date="1560848156" name="ditauEfficiencyPt_mediumTauMVA_2017DataMC.pdf" path="ditauEfficiencyPt_mediumTauMVA_2017DataMC.pdf" size="14987" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_mediumTauMVA_2017DataMC.png" attr="" comment="" date="1560848156" name="ditauEfficiencyPt_mediumTauMVA_2017DataMC.png" path="ditauEfficiencyPt_mediumTauMVA_2017DataMC.png" size="20770" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560848156" name="ditauEfficiencyPt_mediumTauMVA_2018DataMC.pdf" path="ditauEfficiencyPt_mediumTauMVA_2018DataMC.pdf" size="14977" user="egallo" version="1"
META FILEATTACHMENT attachment="ditauEfficiencyPt_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560848156" name="ditauEfficiencyPt_mediumTauMVA_2018DataMC.png" path="ditauEfficiencyPt_mediumTauMVA_2018DataMC.png" size="20708" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyEta_mediumTauMVA_2016DataMC.pdf" attr="" comment="" date="1560848156" name="mutauEfficiencyEta_mediumTauMVA_2016DataMC.pdf" path="mutauEfficiencyEta_mediumTauMVA_2016DataMC.pdf" size="15943" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyEta_mediumTauMVA_2016DataMC.png" attr="" comment="" date="1560848156" name="mutauEfficiencyEta_mediumTauMVA_2016DataMC.png" path="mutauEfficiencyEta_mediumTauMVA_2016DataMC.png" size="19419" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyEta_mediumTauMVA_2017DataMC.pdf" attr="" comment="" date="1560848156" name="mutauEfficiencyEta_mediumTauMVA_2017DataMC.pdf" path="mutauEfficiencyEta_mediumTauMVA_2017DataMC.pdf" size="15997" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyEta_mediumTauMVA_2017DataMC.png" attr="" comment="" date="1560848156" name="mutauEfficiencyEta_mediumTauMVA_2017DataMC.png" path="mutauEfficiencyEta_mediumTauMVA_2017DataMC.png" size="19821" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_mediumTauMVA_2016DataMC.pdf" attr="" comment="" date="1560848156" name="mutauEfficiencyNvtx_mediumTauMVA_2016DataMC.pdf" path="mutauEfficiencyNvtx_mediumTauMVA_2016DataMC.pdf" size="14556" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyNvtx_mediumTauMVA_2016DataMC.png" attr="" comment="" date="1560848156" name="mutauEfficiencyNvtx_mediumTauMVA_2016DataMC.png" path="mutauEfficiencyNvtx_mediumTauMVA_2016DataMC.png" size="20036" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyPt_eachYear_mediumTauMVA_Data.pdf" attr="" comment="" date="1560848209" name="etauEfficiencyPt_eachYear_mediumTauMVA_Data.pdf" path="etauEfficiencyPt_eachYear_mediumTauMVA_Data.pdf" size="15657" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyPt_eachYear_mediumTauMVA_Data.png" attr="" comment="" date="1560848209" name="etauEfficiencyPt_eachYear_mediumTauMVA_Data.png" path="etauEfficiencyPt_eachYear_mediumTauMVA_Data.png" size="26451" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyPt_mediumTauMVA_2017DataMC.pdf" attr="" comment="" date="1560848209" name="etauEfficiencyPt_mediumTauMVA_2017DataMC.pdf" path="etauEfficiencyPt_mediumTauMVA_2017DataMC.pdf" size="14866" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyPt_mediumTauMVA_2017DataMC.png" attr="" comment="" date="1560848209" name="etauEfficiencyPt_mediumTauMVA_2017DataMC.png" path="etauEfficiencyPt_mediumTauMVA_2017DataMC.png" size="20882" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyPt_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560848209" name="etauEfficiencyPt_mediumTauMVA_2018DataMC.pdf" path="etauEfficiencyPt_mediumTauMVA_2018DataMC.pdf" size="14863" user="egallo" version="1"
META FILEATTACHMENT attachment="etauEfficiencyPt_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560848209" name="etauEfficiencyPt_mediumTauMVA_2018DataMC.png" path="etauEfficiencyPt_mediumTauMVA_2018DataMC.png" size="20714" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" attr="" comment="" date="1560848209" name="mutauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" path="mutauEfficiencyEta_mediumTauMVA_2018DataMC.pdf" size="16021" user="egallo" version="1"
META FILEATTACHMENT attachment="mutauEfficiencyEta_mediumTauMVA_2018DataMC.png" attr="" comment="" date="1560848209" name="mutauEfficiencyEta_mediumTauMVA_2018DataMC.png" path="mutauEfficiencyEta_mediumTauMVA_2018DataMC.png" size="19726" user="egallo" version="1"
 
This site is powered by the TWiki collaboration platform Powered by PerlCopyright & 2008-2019 by the contributing authors. All material on this collaboration platform is the property of the contributing authors.
Ideas, requests, problems regarding TWiki? Send feedback