| CMS_btag_DeepFlav_hfstats1_2018 |
uncertainty on b-tagging of udsg and b jets as a linear effect in discriminant score coming from statistical effects in the heavy flavour fit region for the full shape based b-tagging scale factors, separated by year |
btag |
| CMS_btag_DeepFlav_hf |
uncertainty on b-tagging of udsg and b jets from contamination of b and c jets in light flavour fit region for the full shape based b-tagging scale factors |
btag |
| CMS_btag_DeepFlav_lf |
uncertainty on b-tagging of udsg and b jets from contamination of b and c jets in light flavour fit region for the full shape based b-tagging scale factors |
btag |
| CMS_btag_DeepFlav_hfstats2_2016 |
uncertainty on b-tagging of udsg and b jets as a linear effect in discriminant score coming from statistical effects in the heavy flavour fit region for the full shape based b-tagging scale factors, separated by year |
btag |
| CMS_btag_DeepFlav_lfstats2_2016 |
uncertainty on b-tagging of udsg and b jets as a linear effect in discriminant score coming from statistical effects in the light flavour fit region for the full shape based b-tagging scale factors, separarted by year. |
btag |
| CMS_btag_DeepFlav_hfstats1_2016 |
uncertainty on b-tagging of udsg and b jets as a linear effect in discriminant score coming from statistical effects in the heavy flavour fit region for the full shape based b-tagging scale factors, separated by year |
btag |
| CMS_btag_DeepFlav_lfstats1_2016 |
uncertainty on b-tagging of udsg and b jets as a linear effect in discriminant score coming from statistical effects in the light flavour fit region for the full shape based b-tagging scale factors, separarted by year. |
btag |
| CMS_btag_DeepFlav_hfstats1_2017 |
uncertainty on b-tagging of udsg and b jets as a linear effect in discriminant score coming from statistical effects in the heavy flavour fit region for the full shape based b-tagging scale factors, separated by year |
btag |
| CMS_btag_DeepFlav_lfstats1_2017 |
uncertainty on b-tagging of udsg and b jets as a linear effect in discriminant score coming from statistical effects in the light flavour fit region for the full shape based b-tagging scale factors, separarted by year. |
btag |
| CMS_btag_DeepFlav_lfstats1_2018 |
uncertainty on b-tagging of udsg and b jets as a linear effect in discriminant score coming from statistical effects in the light flavour fit region for the full shape based b-tagging scale factors, separarted by year. |
btag |
| CMS_SUS23015_MisIDTTPR |
Prompt rate uncertainties in TT-enriched region. |
custom |
| CMS_SUS23015_MisIDDY1PR |
Prompt rate uncertainties in DY-enriched region with 1 and more jets. |
custom |
| CMS_SUS23015_MisIDDY0PR |
Prompt rate uncertainties in DY-enriched region with 0 jets. |
custom |
| CMS_fake_TT_highpt |
fake rate uncertainty for electrons and muons with high pT in TT-enriched region |
custom |
| CMS_SUS23015_MuWZ0j |
Total number of WZ events with Nj = 0 or 1. |
custom |
| CMS_SUS23015_QCDscale |
Uncertainty from simultaneous variation of qcd renormalization and factorization scales in the WZ and TTZ processes. |
custom |
| CMS_fake_DY_highpt |
fake rate uncertainty for electrons and muons with high pT in DY-enriched region |
custom |
| CMS_SUS23015_ZZ2OnZ0j |
Uncertainties of number of double-onZ ZZ events with different number of jets. |
custom |
| CMS_fake_TT_medpt |
fake rate uncertainty for electrons and muons with medium pT in TT-enriched region |
custom |
| CMS_SUS23015_ZZ2OnZ1j |
Uncertainties of number of double-onZ ZZ events with different number of jets. |
custom |
| CMS_SUS23015_pileup |
pileup uncertainty for 13TeV pp data. |
custom |
| CMS_SUS23015_ZZ2OnZ3j |
Uncertainties of number of double-onZ ZZ events with different number of jets. |
custom |
| CMS_SUS23015_scale_met_unclustered_energy |
total uncertainty on Missing Transverse Energy ffrom unclustered energy in the detector for all years. |
custom |
| CMS_SUS23015_l1_ecal_prefiring |
Uncertainty due to level-1 triggering of bunch crossings before intended trigger for 2016 or 2017. |
custom |
| CMS_fake_DY_medpt |
fake rate uncertainty for electrons and muons with medium pT in DY-enriched region |
custom |
| CMS_SUS23015_eff_m_trigger |
muon trigger efficiency uncertainty for all years. |
custom |
| CMS_SUS23015_eff_e_trigger |
electron trigger efficiency uncertainty for all years. |
custom |
| CMS_SUS23015_eff_m_id |
Additional identification/isolation criteria applied to muons. |
custom |
| CMS_SUS23015_eff_e_id |
Additional identification/isolation criteria applied to electrons. |
custom |
| CMS_SUS23015_ZZ2OnZ2j |
Uncertainties of number of double-onZ ZZ events with different number of jets. |
custom |
| CMS_fake_DY_lowpt |
fake rate uncertainty for electrons and muons with low pT in DY-enriched region |
custom |
| CMS_fake_TT_lowpt |
fake rate uncertainty for electrons and muons with low pT in TT-enriched region |
custom |
| CMS_SUS23015_MuWZ5j |
Formula (rateParam) used to fix number of TTZ or WZ events in separate Nj bins, keeping integral number of these events for Nj > 1. Total number of TTZ or WZ events with Nj > 1 is obtained as a separate nuisance parameter. |
custom |
| CMS_SUS23015_sigmaRjTTZ2to3j |
Uncertainty on Rj value for TTZ or WZ process for various Nj bins. |
custom |
| CMS_SUS23015_sigmaRjTTZ3to4j |
Uncertainty on Rj value for TTZ or WZ process for various Nj bins. |
custom |
| CMS_SUS23015_sigmaRjTTZ4to5j |
Uncertainty on Rj value for TTZ or WZ process for various Nj bins. |
custom |
| CMS_SUS23015_sigmaRjWZ2to3j |
Uncertainty on Rj value for TTZ or WZ process for various Nj bins. |
custom |
| CMS_SUS23015_MuWZ2j |
Formula (rateParam) used to fix number of TTZ or WZ events in separate Nj bins, keeping integral number of these events for Nj > 1. Total number of TTZ or WZ events with Nj > 1 is obtained as a separate nuisance parameter. |
custom |
| CMS_SUS23015_MuWZ3j |
Formula (rateParam) used to fix number of TTZ or WZ events in separate Nj bins, keeping integral number of these events for Nj > 1. Total number of TTZ or WZ events with Nj > 1 is obtained as a separate nuisance parameter. |
custom |
| CMS_SUS23015_MuWZ4j |
Formula (rateParam) used to fix number of TTZ or WZ events in separate Nj bins, keeping integral number of these events for Nj > 1. Total number of TTZ or WZ events with Nj > 1 is obtained as a separate nuisance parameter. |
custom |
| CMS_SUS23015_MuMisIDTTFRnorm |
Normalization of TT-enriched MisID |
custom |
| CMS_SUS23015_MuMisIDDY1FRto5jNorm |
Normalization of DY-enriched MisID with >0 jets. |
custom |
| CMS_SUS23015_MuMisIDDYFR0jNorm |
Normalization of DY-enriched MisID with 0 jets. |
custom |
| CMS_SUS23015_sigmaRjWZ4to5j |
Uncertainty on Rj value for TTZ or WZ process for various Nj bins. |
custom |
| CMS_SUS23015_MuTTZ2j |
Formula (rateParam) used to fix number of TTZ or WZ events in separate Nj bins, keeping integral number of these events for Nj > 1. Total number of TTZ or WZ events with Nj > 1 is obtained as a separate nuisance parameter. |
custom |
| CMS_SUS23015_MuTTZ3j |
Formula (rateParam) used to fix number of TTZ or WZ events in separate Nj bins, keeping integral number of these events for Nj > 1. Total number of TTZ or WZ events with Nj > 1 is obtained as a separate nuisance parameter. |
custom |
| CMS_SUS23015_MuTTZ4j |
Formula (rateParam) used to fix number of TTZ or WZ events in separate Nj bins, keeping integral number of these events for Nj > 1. Total number of TTZ or WZ events with Nj > 1 is obtained as a separate nuisance parameter. |
custom |
| CMS_SUS23015_MuTTZ5j |
Formula (rateParam) used to fix number of TTZ or WZ events in separate Nj bins, keeping integral number of these events for Nj > 1. Total number of TTZ or WZ events with Nj > 1 is obtained as a separate nuisance parameter. |
custom |
| CMS_SUS23015_MuZG |
Normalization of ZG background. |
custom |
| CMS_SUS23015_MuZZ1OnZ |
Normalization of ZZ events with 1 or 2 OnZ pairs. |
custom |
| CMS_SUS23015_MuZZ2OnZ |
Normalization of ZZ events with 1 or 2 OnZ pairs. |
custom |
| CMS_SUS23015_NormTTZ0to1j |
50% uncertainty on normalization of TTZ events with <2 jets. |
custom |
| CMS_SUS23015_NormOthers |
50% uncertainty on normalization of all but major backgrounds. |
custom |
| CMS_SUS23015_MuTTZ2to5j |
Total number of TTZ or WZ events with Nj > 1. |
custom |
| CMS_SUS23015_MuWZ1j |
Total number of WZ events with Nj = 0 or 1. |
custom |
| CMS_SUS23015_MuWZ2to5j |
Total number of TTZ or WZ events with Nj > 1. |
custom |
| CMS_SUS23015_sigmaRjWZ3to4j |
Uncertainty on Rj value for TTZ or WZ process for various Nj bins. |
custom |
| CMS_eff_e |
efficiency uncertainty for electrons for all years. |
electron_efficiency |
| CMS_scale_e |
generic energy scale uncertainty for electrons. |
electron_energy_scale |
| CMS_res_j |
jet energy resolution uncertainty correlated accross all years. |
jet_energy_resolution |
| CMS_scale_j |
single overall jet energy scale uncertainty. |
jet_energy_scale |
| lumi_2017 |
portion of luminosity uncertainty on 13TeV pp data in a given year which is uncorrelated with other Run 2 years. |
luminosity |
| lumi_2016 |
portion of luminosity uncertainty on 13TeV pp data in a given year which is uncorrelated with other Run 2 years. |
luminosity |
| lumi_13TeV_correlated |
portion of luminosity uncertainty on 13TeV pp data which is correlated between 2016, 2017, and 2018 data taking. |
luminosity |
| lumi_13TeV_1718 |
portion of luminosity uncertainty on 13TeV pp data which is correlated between 2017, and 2018 data taking. |
luminosity |
| lumi_2018 |
portion of luminosity uncertainty on 13TeV pp data in a given year which is uncorrelated with other Run 2 years. |
luminosity |
| CMS_eff_m |
efficiency uncertainty for muons for all years. |
muon_efficiency |
| CMS_scale_m |
single energy scale uncertainty for muons for all data-taking periods |
muon_energy_scale |
| CMS_HEM_2018 |
Jet uncertaity due to two HCAL modules whose power supply died during data taking in 2018. |
other_experimental |
| pdf_gg |
maximum deviations from nominal of 100 largest pdf eigenvector variations. |
pdf |