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Completeness: 30%

PAT/ntuples

  • Samples
  •   MC: 311X Monte Carlo samples (even though most of these samples are not at T2's at that moment)
      • Drell-Yan:
        • /DYToMuMu_M-10To20_TuneZ2_7TeV-pythia6/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
        • /DYToMuMu_M-20_CT10_TuneZ2_7TeV-powheg-pythia/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
      • QCD
        • /QCD_Pt-15to20_MuPt5Enriched_TuneZ2_7TeV-pythia6/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
        • /QCD_Pt-20to30_MuPt5Enriched_TuneZ2_7TeV-pythia6/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
        • /QCD_Pt-30to50_MuPt5Enriched_TuneZ2_7TeV-pythia6/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
        • /QCD_Pt-50to80_MuPt5Enriched_TuneZ2_7TeV-pythia6/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
        • /QCD_Pt-80to120_MuPt5Enriched_TuneZ2_7TeV-pythia6/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
        • /QCD_Pt-120to150_MuPt5Enriched_TuneZ2_7TeV-pythia6/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
        • /QCD_Pt-150_MuPt5Enriched_TuneZ2_7TeV-pythia6/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
      • DY tautau
        • /DYToTauTau_M-20_CT10_TuneZ2_7TeV-powheg-pythia-tauola/Spring11-PU_S1_START311_V1G1-v2/GEN-SIM-RECO
      • Dibosons
        • /WWtoAnything_TuneZ2_7TeV-pythia6-tauola/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
        • /WZtoAnything_TuneZ2_7TeV-pythia6-tauola/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
        • /ZZtoAnything_TuneZ2_7TeV-pythia6-tauola/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
      • Wmunu
        • /WtoMuNu_TuneD6T_7TeV-pythia6/Spring11-PU_S1_START311_V1G1-v1/GEN-SIM-RECO
    • DATA: 
      • /MuOnia/Run2011A-PromptReco-v1/RECO (no Mu available)
      • JSONs:
        • "Golden" /afs/cern.ch/cms/CAF/CMSCOMM/COMM_DQM/certification/Collisions11/7TeV/Prompt/Cert_160404-161312_7TeV_PromptReco_Collisions11_JSON.txt
        • Calo-free /afs/cern.ch/cms/CAF/CMSCOMM/COMM_DQM/certification/Collisions11/7TeV/Prompt/Cert_160404-161312_7TeV_PromptReco_Collisions11_JSON_MuonPhys.txt
  • Relevant software: CMSSW_4_1_3,
    • Global tag
      • Data: GR_R_311_V2 for reprocessing and GR_P_V14 for prompt reco
      • MC: MC_311_V2, START311_v2
    • ElectroWeakAnalysis/Skimming, ElectroWeakAnalysis/DYskimming, UserCode
  • how to run:  PATtuple production: see the corresponding twiki, note, a lot of code in CVS is outdated (we keep updating it)
    cmsrel CMSSW_4_1_3
    cd CMSSW_4_1_3/src
    cmsenv
    addpkg ElectroWeakAnalysis/Skimming
    cvs co -d ElectroWeakAnalysis/DYskimming -r V00-00-05 UserCode/Purdue/DYAnalysis/Skimming
    scram b

Event Selection

  • Mass range and binning:

    • for the early stage of 2011 analysis we keep the 2010 binning [15,20,30,40,50,60,76,86,96,106,120,150,200,600]

    • Based on the analysis of trigger thresholds and acceptance/significance curves we will reoptimize the lower mass edge.
    • Higher mass edge will be determined by the highest mass dimuons available in the dataset
    • It is possible that statistics will allow to make bins finer
  • Online: HLT_Mu15_* || HLT_Mu24_* (by run range), HLT_DoubleMu7_*
  • Offline: Baseline event selection has not changed compared to 2010 analysis, see
    • we will consider moving to PF muons and PF isolation
  • Relevant software: ROOT macros for control plots and invariant mass plot are here: UserCode/Purdue/DYAnalysis/AnalysisMacros/ControlPlots

Acceptance

  • Acceptance is determined using GEN level information, which has not changed compared to the 2010 analysis
  • Use the acceptance numbers documented in the note: AN-11-013

We use POWHEG NLO acceptance, see all the relevant formulas in this talk (the updated version), see slide18 for acceptance definitions and refer to earlier talks. Di\ue to the intrinsic discrepancies in the modeling between the POWHEG and FEWZ we correct the Z kinematics. For that, we extract the weight maps from POWHEG at NLO and from FEWZ at NNLO (to be more specific it is at NNLO below 40 GeV and NLO otherwise, as the effect of higher order corrections is negligible at the higher masses). The weight map is essentially the ratio of double inclusive cross-sections extracted from POWHEG and FEWZ per PT-Y bin (PT, Y refer to Z kinematics, which is identical here to dimuon kinematics, our final aim). Details on the re-weighting technique are also in the linked presentation.

How to run: The code makes use of mostly Adam's tools. Current working area is here: /home/ba01/u115/asvyatko/PATAdam/CMSSW_3_8_7/src

To setup area do:

cmsrel CMSSW_3_8_7
cd CMSSW_3_8_7/src
cmsenv
cvs co -r V00-09-11 SUSYBSMAnalysis/Zprime2muAnalysis
SUSYBSMAnalysis/Zprime2muAnalysis/setup.csh # This last command checks
                                            # out other packages and
                                            # executes scramv1 b to
                                            # compile everything.
cvs co -d Acceptance /UserCode/ASvyatkovskiy/AcceptanceAdam

Not yet tested under CMSSW 4XY, because there was no need - GEN level info did not change. Follow README to calculate weights, which also calculates the 1D acceptance in mass bins.

Weight map producer uses the FEWZ acceptance as the input, find all the macros here: /UserCode/ASvyatkovskiy/FEWZ_scripts,

to work one needs to do*:*

cd $RCAC_SCRATCH/
cp -r /home/ba01/u115/asvyatko/TEST_FEWZ/FEWZ_2.0.1.a3/ YOUR_FEWZ_WORKING_DIR
cvs co -d TMP /UserCode/ASvyatkovskiy/FEWZ_scripts
cp TMP/* .
rm -r TMP

To run you use whatever config you need python nu_create_*.py.

Efficiencies

The details on the factorization and the application of correction factors are documented here , and can be found in this talk

  • Trigger, Reconstruction: TagAndProbe, official package
  • How to run (on top of CMSSW 414): 
    addpkg MuonAnalysis/MuonAssociators V01-14-00
addpkg PhysicsTools/PatUtils
addpkg PhysicsTools/TagAndProbe V04-00-06
cvs co -A MuonAnalysis/TagAndProbe
    • The procedure goes in two steps:
      • T&P tree production -> rerun seldom (ideally once), it depends only on the definitions of the tag and probe
      • fitting: separate job for trigger and all the muonID related efficiencies -> reran frequently and usually interactively (change binning, definitions)
    • All the latest macros/configs can be found here: UserCode/ASvyatkovskiy/TagAndProbe
  • Isolation: RandomCone - contacted Alexey D asking for a recipe.

Background estimation

There are various methods employed to estimate the QCD background in a data-driven way (QCD is currently the only background estimated not from MC). These are

Unfolding

FSR corrections

Systematic uncertainties

Final Plots

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