Difference between revisions of "Aod ntuple"

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== Electron ==
 
== Electron ==
  
{| border="0" cellpadding="10" cellspacing="10"
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{| border="1" cellpadding="10" cellspacing="10" style="border-collapse: collapse; border: 5px solid orange"
 
|+ ''' Electron in AOD/Ntuple '''
 
|+ ''' Electron in AOD/Ntuple '''
 
|-  
 
|-  
| AOD Container Name || AOD Variable || Ntuple Variable || Comment
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| AOD Container Name  
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| AOD Variable  
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| Ntuple Variable
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| Comment
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| ElectronCollection
 
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Revision as of 12:20, 19 May 2005

This page contains basic prescriptions to get physics objects from the AOD and the AOD-based Root ntuple.

Some comments on quality selection cuts will be added as work progresses.


Electron

Electron in AOD/Ntuple
AOD Container Name AOD Variable Ntuple Variable Comment
ElectronCollection

There are 3 types of quality cuts you can perform on the electron candidates:

  1. Cuts based on the isEM flag
  2. Cuts based on likelihood
  3. Cuts based on NeuralNet output

1. The isEM flag uses both calorimeter and tracking information in addition to TRT information. The flag is a bit field which marks whether the candidate passed or not some safety checks.

The bit field marks the following checks:

  Cluster based egamma
  ClusterEtaRange        =  0,
  ClusterHadronicLeakage =  1,
  ClusterMiddleSampling  =  2,
  ClusterFirstSampling   =  3,
  Track based egamma
  TrackEtaRange          =  8,
  TrackHitsA0            =  9,
  TrackMatchAndEoP       = 10,
  TrackTRT               = 11

In 9.0.4 there is a problem with TRT simulation so one has to mask TRT bit to recover the lost efficiency.

To get the flag in your AOD analysis you should use:

(*elec)->isEM()

To mask the TRT bits you should use: (*elec)->isEM()&0x7FF==0

If you use isEM then you will select electrons with an overall efficiency of about 80% in the barrel but much lower in the crack and endcap.

2. The likelihood ratio is constructed using the following variables: energy in different calorimeter samplings, shower shapes in both eta and phi and E/P ration. No TRT information is used here. You need to access two variables called emweight and pionweight then you can construct the likelihood ratio, defined by: emweight/(emweight+pionweight).

In AOD, you use the following code:

ElecEMWeight = elec*->parameter(ElectronParameters::emWeight); ElecPiWeight = elec*->parameter(ElectronParameters::pionWeight);

Then form the variable: X = ElecEMWeight/(ElecEMWeight+ElecPiWeight);

Requiring X > 0.6 will give you more than 90% efficiency for electrons.


3. The NeuralNet variable uses as inputs the same variables used for likelihood. To use it in AOD you should proceed as follow:

ElecepiNN = elec*->parameter(ElectronParameters::epiNN);

Requiring ElecepiNN > 0.6 will give you about 90% eff for electrons.

However, you should be aware that the NN was trained in full eta range while the likelihood was computed in 3 bins in eta: barrel, crack and endcap. So I would suggest to use likelihood for now.

Muon

Tau

Jet

BJet

Missing Et

External References

Container/Object Names for AOD

Particle Preselection Cuts