Version 16 (modified by 7 years ago) ( diff ) | ,
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The first MadAnalysis 5 workshop on LHC recasting @ Korea
Analysis 8: ATL-PHYS-PROC-2O16-117
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Supervisor(s) | Eric Conte | Benjamin Fuks |
1. Analysis summary
A measurement of the tt¯Z and tt¯W production cross sections in final states with:
- two same-charge muons: one muon coming from Z/W and one from the top decay.
- or three leptons (electrons or muons),
- or four leptons (electrons or muons): only ttZ case where Z and the 2 top quarks are decaying leptonically.
The analysis uses a data sample of proton-proton collisions at s√=13 TeV recorded with the ATLAS detector at the Large Hadron Collider in 2015, corresponding to a total integrated luminosity of 3.2 fb−1. The inclusive cross sections are extracted using likelihood fits to signal and control regions, resulting in σtt¯Z=0.9±0.3 pb and σtt¯W=1.5±0.8 pb, in agreement with the Standard Model predictions.
2. Analysis global information
- ATLAS contact person: nobody
- Center of mass energy: 13 TeV
- Integrated luminosity: 3.2 fb−1
- Link to arXiv: https://arxiv.org/abs/1609.01599
- Link to the collaboration page: https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/TOPQ-2015-22/
- Link to CDS: https://cds.cern.ch/record/2211022?ln=fr
- Link to Inspire: http://inspirehep.net/record/1485353
- Link to Rivet analyses: https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2016-005/
3. Selection description
3.1 Trigger selection
Only events using single-electron OR single-muon triggers are accepted:
- single-electron: one electron with pT > 24 GeV
- single-muon: one muon with pT > 20 GeV
PS: This part cannot usually be described by the fast-simulation of detector.
3.2 Object definition
- electron:
- pT > 7 GeV,
- |eta|<2.47. Are excluded electrons in the end-cap, i.e. 1.37 < |eta| < 1.52.
- 'medium' likelihood identification.
- transverse impact parameter: |d0|/err(d0) < 5.
- longitudinal impact parameter: |z_0 x sin\theta | < 0.5 mm
- isolation criterion:
- sum PT of tracks in a cone around the electron (the electron track is subtracted) of size = min(10 GeV/PT,0.2) < 6% electron PT.
- sum ET of clusters in a cone around the electron (the electron cluster is subtracted) of size DR=0.2 < 6% electron PT.
- muon:
- pT > 7 GeV
- |eta|<2.4
- 'medium' identification.
- transverse impact parameter: |d0|/err(d0) < 3.
- longitudinal impact parameter: |z_0 x sin\theta | < 0.5 mm
- isolation criterion: sum PT of tracks in a cone around the muon (the muon track is subtracted) of size = min(10 GeV/PT,0.3) < 6% muon PT.
- jet:
- clustering: anti-kT with =0.4
- pT > 25 GeV
- |eta|<2.5
- Pile-up rejection: jets with pT < 60 GeV and |η| < 2.4 are required to satisfy pile-up rejection criteria (JVT)
- b-jet: MV2c20 algorithm. In simulation, the tagging algorithm gives a rejection factor of about 130 against light-quark and gluon jets, and about 4.5 against jets containing charm quarks.
- preventing double-counting:
- the closest jet within DR=0.2 cone of an electron is removed.
- if, after the previous selection cut, the nearest jet of an electron is in DR=0.4 cone, then the electron is removed.
- muons in a DR=0.4 cone around a given jet are removed. BUT if the jet has fewer than three associated tracks, the muon is kept.
3.3 Cut-flow chart
- Common:
- 0. Trigger confirmation: at least one lepton (muon/electron) with PT > 25 GeV
- 1. Analysis 1: SS-muons
- 1.1. 2 muons of same charge, with PT > 25 GeV
- 1.2. Events with additional leptons are vetoed
- 1.3. MET > 40 GeV
- 1.4. HT > 240 GeV
- 1.5. At least 2 b-jets
- 2. Analysis 2: trilepton analysis
- 2.1. Exactly 3 leptons
- 2.2. 2 opposite sign, same flavour leptons, and
- 2.2. Leading lepton with PT > 25 GeV, the other leptons with PT > 20 GeV
- 2.3. Defining 4 signal regions according the final states:
- 3l-Z-1b4j
- 3l-Z-2b3j
- 3l-Z-2b4j
- 3l-noZ-2b
- 2.4. Compatibility with a Z:
- [3l-Z-1b4j]+[3l-Z-2b3j]+[3l-Z-2b4j]: compatible with a Z i.e. (invM-MZ)<10 GeV
- [3l-noZ-2b]: not compatible with a Z i.e. (invM-MZ)>10 GeV
- 2.5. Number of light jets (no b-jet):
- [3l-Z-2b3j]: #jets = 3
- [3l-Z-1b4j]+[3l-Z-3b4j]: #jets >= 4
- [3l-noZ-2b]: #jets = 2, 3 or 4
- 2.6. Number of b-jets:
- [3l-Z-1b4j]: #b-jets = 1
- [3l-Z-2b3j]+[3l-Z-3b4j]+[3l-noZ-2b]: #b-jets >= 2
- 3. Analysis 3: tetralepton analysis
- 3.1 Exactly 4 leptons
3.4 Definition of exotic observables
Like SUSY transverse observable. Notice that classical MT2 & MT2W are encoded within the MadAnalysis framework.
3. Detector simulation
Can we use the last release of the Delphes package with the CMS/ATLAS MA5tune-card? or do need to improve the simulation?
4. Validation material
4.1 Monte-Carlo samples
- LO/NLO?
- Model used:
- MC generator program (name + version):
- Shower program (name + version):
- Tune of Pythia:
- PDF set:
- ME/PS merging????
4.2 Reference plots / cut-flows
- List of validation material