Title: Jet efficiencies experience at D
 1Jet efficiencies experience at DØ
- Jet ID 
 -  Choose energy to be clustered into jets 
 -  Choose clustering algorithms and parameters 
 -  Choose sets of selection criteria 
 - Prepare  optimize jet ID tools 
 - Choose a basic set of cuts 
 - Fancier optional cuts (e.g. jet-vertex matching) 
 -  Measure reconstruction and selection 
efficiencies  - For this talk Ill concentrate on measuring 
reconstruction and selection efficiencies,  - Known in DØ as jet certification (4)
 
- Amnon HarelUniversity of Rochester
 
  2Jet certification timeline
Reviewingbasicassump-tions 
First fullcertification
1st use of conclusions
Several early measurements
2nd fullcertification
First (preliminary) results with jets
This data published with methodologiesdescribed 
in this talk 
 3The theme
- Concentrating aspects relevant to LHC. 
 - The recurring theme 
 - Limited resolution makes significant bias 
possible  -  large (exponential) slope dont help either
 
  4An example
- The natural way to measure jet ID efficiency is 
to take your data sample, and bin isGood in the 
jet pT. But theres a bias  layer fractions (EMF 
and CHF) are correlated to the energy scale and 
resolution. 
These are the same di-jet events, using a fully 
efficient trigger. Red  EMF of the jet with 
130(unbiased).
The bias increases the high EMF inefficiency by 
100-400 
 5Jet Reconstruction Eff.
- The point of a reconstruction eff. measurement is 
that the probe jet may not exist!  -  Need a tag  probe procedure to identify events 
where were sure the jet should exist, even if 
the detector says no.  -  Need a tag track to find the ? of the jet 
 -  Must trust MC to model how this criteria effects 
jet efficiencies ?  
- Possible samples 
 -  Zjets  good sE - fairly pure  sideband 
subtractions possible  low statistics  -  ?jets  good sE  impure  high statistics  
 -  backgrounds have unusual JES (neither ? nor 
generic jets!)  -  di jets  bad sE  very pure  high statistics 
 - We will see that having a good tag sE is an 
illusion  - ? Di jets are by far the best sample for jet 
reconstruction efficiency measurements 
  6Hemisphere imbalance
- Contrary to popular belieftwo object production 
is NOT balanced in pT  - That is only true on average 
 - The spread is 4-5 GeV for any axis (at the 
Tevatron)  - update of hep-ph/9808467 with hep-ex/0412050 by 
M.Begel  - Theory due to the pT carried by the partons 
(neglected in naïve PDF picture)  - Experiment beam remnants carry significant pT 
down the beam pipe  - Hence even with infinite precision on the tag 
energy, the resolution of the predicted probe pT 
will be no better than 4 GeV, which is enough for 
an interesting (?) bias  - ?Good sE on the probe is an illusion 
 - Is this of any numerical importance?
 
  7Jet reco. Naïve tag  probe
- The natural way to measure jet reco. efficiency 
is to take your tag  probe sample, and bin 
events in the tag jet pT. Then 
In terms of passing or failing jet reco.
In terms of  of tags and  of probes
Only one problem This gives completely the wrong 
results Do you see the mistake? 
 8The 1st red flag
MC
MC
No jet
With jet
Data vs. MCdiscrepancies ?Irrelevant
No jet
With jet
Data
Data
Naïve method assumesthese pTs are the same! 
 9Toy MC 
 10Toy MC - II 
 11Jet ID Eff.
Tag probe jet exists Probe jet ID
- Jet ID is easier  can tag dijet events and probe 
jet ID  -  No need for a track 
 - Why bother with tag  probe? 
 - To get pT dependence of jet ID eff. despite the 
jet ID  E bias shown on slide 4 
Tag jet
Possible samples Same discussion as for jet 
reco. eff.  di jets are best 
 12Conclusions
-  Limited resolution makes significant bias 
possible  - Imposing pT bins ? bias 
 - Requiring that a jet is or is not reconstructed ? 
different biases  - Requiring that a jet pass jet ID ? bias 
 -  Contrary to popular belief two object 
production is NOT balanced in pT  - That is only true on average 
 - The RMS is 5-6 GeV at the LHC (4-5GeV at the 
Tevatron)  -  It is not straightforward to measure pT 
dependent jet reco. eff.  - Can not correct the results of the naïve 
approach  - Difficult to fit from observable spectra 
 - Might be possible by unbiasing (and smoothing) 
the pT dependence of the pass and fail samples 
before combining them into an efficiency  - Probably dominated by energy resolution anyways ? 
just get that right ?  -  Jet ID eff. are fairly easy to measure 
 - Tag  probe needed to avoid jet ID ? E bias
 
  13  14?
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