Difference between revisions of "Aod ntuple"

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| Number of hits in the TRT
 
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| Algorithm used to create the electron: <code>softe</code> or <code>egamma</code>  
 
| Algorithm used to create the electron: <code>softe</code> or <code>egamma</code>  
 
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| Energy deposition in a cone dR=0.45 around the electron cluster
 
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| Energy deposition in a cone dR=0.20 around the electron cluster. Standard cone size for ATLFAST
 
| Energy deposition in a cone dR=0.20 around the electron cluster. Standard cone size for ATLFAST
 
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| Energy deposition in a cone dR=0.30 around the electron cluster. Currently empty
 
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| Energy deposition in a cone dR=0.40 around the electron cluster
 
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| Weight for electrons (see below)
 
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Revision as of 13:44, 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 Variable Type Comment
ElectronCollection n_elec Int Number of electrons in the Ntuple
px_elec Double Px
py_elec Double Py
pz_elec Double Pz
pt_elec Double Pt
eta_elec Double Eta
phi_elec Double Phi
isem_elec Int isEM flag (see below)
hastrk_elec Int (bool) HasTrack flag: presence of charged track in the Inner Detector
z0vtx_elec Double Intersection (z) of track with the beam axis
d0vtx_elec Double Transverse impact paramter d0
nblayerhits_elec Int Number of hits in the Pixel B-layer
npixelhits_elec Int Number of hits in the Pixel detector
nscthits_elec Int Number of hits in the SCT
ntrthits_elec Int Number of hits in the TRT
ntrththits_elec Int Number of high threshold hits in the TRT
auth_elec Int??? Algorithm used to create the electron: softe or egamma
eoverp_elec Double E/P ratio
etcone_elec Double Energy deposition in a cone dR=0.45 around the electron cluster
etcone20_elec Double Energy deposition in a cone dR=0.20 around the electron cluster. Standard cone size for ATLFAST
etcone30_elec Double Energy deposition in a cone dR=0.30 around the electron cluster. Currently empty
etcone40_elec Double Energy deposition in a cone dR=0.40 around the electron cluster
emwgt_elec Double Weight for electrons (see below)
piwgt_elec Double Weight for pions (see below)

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.

Photon

Muon

Tau

Jet

BJet

Missing Et

External References

Container/Object Names for AOD

Particle Preselection Cuts