More details to be found here: TopJetLiaisonR172Recommendations
AntiKt4LCTopoJets
collection (D3PD name jet_AntiKt4LCTopoJets_bla
e.g. jet_AntiKt4LCTopoJets_eta
). ApplyJetCalibration
tool.
We suggest to cut at: |JVF| >0.5
(wrt 0.75 for
2011, allows us to be consistent with other groups and b-tagging
calibrations)
Further studies on the cut values, SF and possibly additional systematics are being carried out by the JetEtmiss group.
If electron is reconstructed inside a real jet, the energy is double counted. One solution is to remove electron clusters (or cells) and re-do jet reconstruction. This is a longer term task. Note that "simple" solutions, such as vetoing such miscreconstructed events, creates new problems and does not seem to be an improvement. See e.g. this thread. The current recommendation is to do nothing about the energy double counting. This is fine as long as the effect is reproduced by the simulation.
Jets used for the analysis are AntiKt4Topo jets. For analysis aiming for Top 2012, we stick with EM+JES calibrated jets. Everyone else should move already now to LC jets.
General information on re-applying the jet calibration is at JetCalibrationToolsForPhysicsAnalyses and JetStudies2012.
Note that for LC+JES jets (e.g. AntiKt4LCTopo), make sure that instead of the emscale variables you are using the constscale variables. This is because the scale at which the JES has been derived already assumes that the clusters have been calibrated with the LCW scheme.
Also note that currently, origin-corrected eta and phi should not be used.
Note that after the jet calibration is applied, the entire 4 vector of the jet can change. We propagate the change in pt to recalculate the MET, but keep the jet direction the same.
More information on how to use the uncertainty provider tool is available at JetUncertainties2012.
You should always use calibrated quantities
after the ApplyOffsetEtaJES
macro to evaluate the
JES uncertainty, and rescale the energy components of the
four-vector (E and pT, but the mass will change as well) using the
uncertainty factor.
No smearing of the nominal MC jets is needed; smearing needs only to be done to obtain the systematic uncertainty on your final measurement.
Use ApplyJetResolutionSmearing-00-01-00 and JetResolution-02-00-00. Further instructions
at JetEnergyResolutionProvider2012 and ApplyJetResolutionSmearing.
Jet cleaning has to be applied to both data and Monte Carlo, and it is recommended to use the IsBadLooseMinus flag (=branch) in NTUP_TOP.
Events should be rejected if there is a bad jet with pt>20
GeV.
For the sake of consistency among analyses we recommend to cut on
the fully corrected jet pt after recalibration (i.e. the pt used
in the analyses)
Further recommendations are available at HowToCleanJets2012.
NOTE : To obtain the last set
of SF, you have to choose the year argument as 2012mc12a
(and not 2012 anymore).
IMPORTANT! The SFs have been extracted after applying the additional mu re-weighting described in the InDetTrackingPerfo page. It is very important that you make sure you apply that to your analysis, too, before using the SF.