Multivariate Analysis for Z eμ
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Transcript of Multivariate Analysis for Z eμ
Multivariate Analysis for Zeμ
Kyoko Yamamoto Iowa State University
8TeV eμ/eτ/μτ
LFV resonance search meeting January 22, 2013
MC12 Zeμ Sample Request• Job option file:
MC12.180333.Pythia8_AU2MSTW2008LO_Zemu_LeptonFilter.py • Generator: Pythia 8.165 • Filter efficiency: 0.62291
– Lepton filter: pT(l) > 5GeV, |η(l)| < 2.8, and N(l) = 2
• Number of events: 50K (10 files)
• Full simulation• Zeμ validation wiki page including validation plots: https://
twiki.cern.ch/twiki/bin/viewauth/AtlasProtected/LFVinZemu• Savannah request URL: https://savannah.cern.ch/task/?38680
– Request has been approved, and simulation will be running soon
• Using my private full simulated Zeμ sample (50K events) without the lepton filter until the official sample is available
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Event Selection• Trigger (unprescaled for all periods)
– Electron: EF_e24vhi_medium1 || EF_e60_medium1
• Good Run Lists for data only• Vertex: primary vertices associated with more than 3 tracks • Data quality: veto LAr noise burst, Tile corrupted, or incomplete events• Jet cleaning (cleaning should be applied to AntiKt4TopoEM jets)
– Use only jets that survive the lepton overlap removal (remove jets with ΔR < 0.3 to SELECTED electrons/muons)
– Remove events with at least one LOOSE bad or ugly jet with pT (calibrated jet) 20GeV for ≧both data and MC (jet_isBadLooseMinus, jet_isUgly)
– Hot tile calorimeter cleaning for data only– FCal cleaning for both data and MC
• Exactly one high pT isolated tight e and one high pT isolated combined μ
• Veto events with 2nd high pT “no isolation required” loose electron or combined muon
• Trigger matching• Opposite charge of electron-muon pair
• Invariant mass: 66 < Meμ < 116 GeV
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Not applied |Δφ(e,μ)| > 2.7 at this time
Dilepton Mass Distribution
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• Signal (Zeμ) corresponding to the LEP1 BR limit (BR < 1.7×10-6) is overlaid with the stuck background histogram
• Our MVA analysis does not include QCD background, but QCD is small• NOS(QCD) ~ NSS(QCD)
• W+jet sample shows statistical fluctuations
Opposite charge pair Same charge pair
MET and Jet Distributions in 86 < M(eμ) < 96 GeV (Z-mass Pole)
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More plots: http://hep-int1.physics.iastate.edu/~kyoko/IowaState/Zemu/
Missing transverse energy Transverse momentum for leading jet
Multivariate Analysis (MVA)
• TMVA (Toolkit for MVA) – ROOT-integrated machine learning
environment for the processing and parallel evaluation of multivariate classification and regression techniques
– Including many multivariate methods
• Boosted Decision Trees (BDT)– Sequential application of cuts splits
the data into nodes, where the final nodes classify an event as signal or background
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Ref: Helge Voss, “Decision Trees and Boosting,” TMVA Workshop , CERN, 21 Jan 2011
Variables for MVA
• Picking up some variables to test MVA although some variables are correlated– Missing transverse energy
• Using MET_RefFinal_STVF after the MET correction
– Leading jet pT (if no jets, pT(1st jet) = 0)• Using AntiKt4LCTopo jets after the jet calibration
– AntiKt4LCTopo improves the resolution and is recommended by the Jet/EtMiss group and Arantxa (SM Jet convener)
– Number of jets for pT(jet) > 20GeV and |y| < 4.5
– Azimuth angle between electron and muon: Δφ(e,μ)
– Dilepton pT(eμ)
– pT(e) (after pT(e) > 25GeV cut)
– pT(μ) (after pT(μ) > 25GeV cut)
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Correlation MatrixBackground Data
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data
• Some variables are highly correlated as we expected• pT(jet) and N(jet), Δφ(e,μ) and pT(eμ)
MVA Response: BDT
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Background shape for BDT response agrees with data well
Tested signal and backgroundTested background and applied the
BDT result to data
Signal and Background Efficiencies
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High background rejection at high signal efficiency It looks good!