IFAEAtlasAnalysis
Introduction
This page is created by IFAE Barcelona. It is supposed to collect or share useful information about ATLAS analysis.
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Useful links
- IFAE Cvs Repository IFAECvsRepo
- CSC data
- Grid
- Analysis tools
- MC production
- General information
Trigger
Z+jets
Object ID
Electron Reconstruction
- Short description and Documentation
- I'm starting documentation in EventViewElectronDetailed, but this will take some time..
- As long as the CSC note is not finished, the best EMID documentation can be found in the EgammaATLASRecoPerformance page. Here you can find the link to the most recent performance note
.
- A complete list of the AOD content can be accessed from the Class references in the AOD pages
- A project to document the AOD content has started (Kevin Black). So far the mosy useful documentation is the EgammaCBNT page and the documentation of the most important Electron Variables produced by the EV calculators in 12.0.x
- Electron candidates are separated in reconstruction from Photon candidates by applying a loose track match. The default electron ID uses a hollow cone isolation and the IsEM flag which is composed of bits that correspond to various requirements on the shower shape in the calorimeter and the track in the ID (see ElectronGammaIsEM page). Alternative approaches using multivariate techniques (NN, Likelihood, HMatrix, ..) are in advanced stage of development.
- A good source of information are also various recent talks in the EMID group
- More details about the Electron ID
- AOD electron :
- Sliding Window Clusters in 5x5, 3x5 and 3x7
- Clusters corrected for position and energy modulations
- Separation of Electron and Photon candidates by a simple track match: DEta<0.025 , DPhi<0.05; E/p<4
- Hadronic activitity < 20%
- Is EM is calculated (no cut applied in AOD), using information about the Hadronic Leakage, the lateral shower shape in the second sampling of the EM Calorimeter, the lateral shower shape in the strips, the track Quality Cuts (# of hits and impact parameter), the track-calorimeter spatial matching, E/p and the fraction of high threshold TRT hits
- The electron likelihood parametrizes the distributions of various discriminating variables for signal (S) and background (B) which are then interpreted as PDFs. The signal probability S ( or
em Weight
) and the background probability B (or pion Weight
) are calculated as a product of the individual probabilities. The final discriminant is the likelihood ratio S/(S+B). The ATLAS electron likelihod uses e0/e, e1/e, e2/e, e3/e, Et Cone40/et, E237/E277, E233/E237,et/(et+Etha), e/p, deta1, dphi2, zvertex/errz, Weta1, Weta2, E2tsts1-Emins1, Fracs1, Isol and numtracks (see documentation of vaiables )
Muon Reconstruction
Jet Reconstruction
MC data sets
- Pythia Z-> leplep inclusive
- Documentation
- Z->ee: 5144
trig1_misal1_csc11.005144.PythiaZee.recon.AOD.v12000601
- Z->mumu: 5145
trig1_misal1_csc11.005145.PythiaZmumu.recon.AOD.v12000601
- Z->tautau->lep: 5146
trig1_misal1_csc11.005146.PythiaZtautau.recon.AOD.v12000601
- Higgs group Z+jets Loose samples:
- Information:
- ID 8130 .... 8135 (0 jets .... >=5 jets)
- atlfast samples:
/castor/cern.ch/grid/atlas/users/jtanaka/HiggsWG/Z_samples/fast/CBNT/
- fully reconstructed Zee:
trig1_misal1_mc12.008131.AlpgenJimmyZeeNp1LooseCut.recon.AOD.v12000601
etc.
- fully reconstructed Zmm:
trig1_misal1_mc12.008143.AlpgenJimmyZmumuNp1LooseCut.recon.AOD.v12000601
etc
- Alpgen Susy background: Z->nunu
- Information: ZplusJetsAlpgen
- ID: 8124 ... 8129
- atlfast samples (directory contains also other SUSY background ):
/castor/cern.ch/grid/atlas/datafiles/susy/atlfast/2006_b
- QCD background
- for Zmm:
trig1_misal1_mc12.017506.PythiaB_bbmu6mu4X.recon.AOD.v12000601
- for Zee:
trig1_misal1_mc12.005802.JF17_pythia_jet_filter.recon.AOD.v12000601
- Pythia SUSY background
Zmumu+jets analysis
TTbar-> tau
MC samples
- Top MC samples are defined here. Any sample reconstructed with release 11 can found at panda monitor
. Production with release 12 is on going, not much was produced until now (for Top analysis), however some few AODs were reconstructed by Elzbieta, and can be found at:
- W->e nu: 5104 = /castor/cern.ch/grid/atlas/users/ashibata/cscpre12-5104
- Z->tautau: 5188 = /castor/cern.ch/grid/atlas/users/ashibata/cscpre12-5200
- ttbar: 5200 = /castor/cern.ch/grid/atlas/users/ashibata/cscpre12-5200
- single top: 5501 = /castor/cern.ch/grid/atlas/users/ashibata/cscpre12-5200
- And replicated at pic at:
- /nfs/atlas-data03/cosuna/official_data/cscpre12/csc11.005200.T1_McAtNlo_Jimmy.digit.RDO.v11004205
- As the statistics for rel12 is not enough, we reconstructed more events (running on rel11 digit files) and placed them under:
- /nfs/atlas-data03/cosuna/official_data/cscpre12/csc11.005200.T1_McAtNlo_Jimmy.digit.RDO.v11004205_IFAE
- Ntuples produced with the leptonic W's daughter-number fix are placed under:
- /nfs/atlas-data03/fiorini/cspre12/ntuples
TopViewAANtuple.new.root
has been obtained merging the 2 other files.
TopView ntuples
B-tagging
B tagging is done by default combining the results of 2 different algorithms:
IP3D and SV1.
- IP3D calculates with tracks informations the 3-D impact parameter (
d
) of a b vertex candidate and its significance: s = d/sigma(d)
.
- SV1 reconstructs secondary vertices in the BJet. SV1 algorithm uses a bottom-up approach: it fits vertices with all pairs of tracks, retaining the fit with the highest probability and fitting the remaining tracks of the jet to this vertex. All tracks below a certain fit probability will be rejected. A likelihood variable is calculated with the secondary vertex parameters (mass, fit probability, multiplicity and distance from the reconstructed primary vertex).
- The two informations are summed in a bjet weight variable, that is variable used to discriminate bjets from other jets. The standard cut on the weight is at value of 3 (b-tagged jets having a weight greater than 3). The cut can be changed in TopView inside
python/TopViewInserters_module.py
. The default tagging algorithm has an efficiency of 60% and a Rejection factor for light jets of 240 in ttjjenu and ttH events.
- More details are available at BTagging Homepage and the main BTagging algorithm is in CVS under:
PhysicsAnalysis/JetTagging/JetTagAlgs/BTagging
- ...
SUSY
Links
Data
EV groupArea at PIC.
The
PAT group is continuosly developing and applying patched to official atlas releases, even when the release is out. Therefore they make use the so called groupArea, where they install updates packages that will overload the default packages to be found in the release. In order to use the latest EV, SUSYView,
TopView,... we need to install a given EVTag at PIC (exactly in the same way as they do in groupArea at CERN). There are several ways one can do that (consult
here), but the easiest and faster is to use pacman.
I installed the latest EV version at:
/nfs/pic.es/user/c/cosuna/scratch/public/EVgroupArea/EventView-12.0.4.3
In order to use this area, prepend this path to your CMTPATH before running athena:
export CMTPATH=/nfs/pic.es/user/c/cosuna/scratch/public/EVgroupArea/EventView-12.0.4.3:$CMTPATH
Future updates can be installed in the same
EVgroupArea directory using pacman
Let say you want to install
EventView-$Release at PIC. First configure pacman:
* cd /nfs/pic.es/user/c/cosuna/scratch/public/pacman/pacman-$VERSION
* source setup.sh
Then go to the EV groupArea directory and create a new directory for the desired version
* cd /nfs/pic.es/user/c/cosuna/scratch/public/EVgroupArea/
* mkdir EventView-$RELEASE
* cd EventView-$RELEASE
and execute the pacman command:
* pacman -v all -get http://atlas-computing.web.cern.ch/atlas-computing/links/kitsDirectory/PAT/EventView/:EventView-$RELEASE.pacman
Bibliography
Under this section are stored some interesting documents, talks and lectures that you can find helpful to consult during your analysis:
Major updates:
--
UllaBlumenschein - 09 Jan 2007
-- Main.cosuna - 09 Jan 2007
%RESPONSIBLE% Main.unknown
%REVIEW%
Never reviewed