/MuHad/Run2012A-22Jan2013-v1/AOD, CMS collaboration
Cite as: CMS collaboration (2022). MuHad primary dataset in AOD format from Run of 2012 (/MuHad/Run2012A-22Jan2013-v1/AOD). CERN Open Data Portal. DOI:10.7483/OPENDATA.CMS.EM42.N900
Dataset Collision CMS 8TeV pp CERN-LHC
MuHad primary dataset in AOD format from RunA of 2012. Run period from run number 190456 to 193621.
The list of validated runs, which must be applied to all analyses, can be found in
CMS list of validated runs Cert_190456-208686_8TeV_22Jan2013ReReco_Collisions12_JSON.txt
docker.io/cmsopendata/cmssw_5_3_32-slc6_amd64_gcc472:latest
gitlab-registry.cern.ch/cms-cloud/cmssw-docker-opendata/cmssw_5_3_32-slc6_amd64_gcc472:latest
Events stored in this primary dataset were selected because of the presence of at least one or two isolated high-energy muons. They also have either high scalar sum of the jet transverse momenta (HT); or the requirement of a loose hyperbolic cut on razor variables, like R2 and MR, defined in terms of the momentum of two megajets; or one or more central jets; or high missing transverse momentum from jets and a high scalar sum of the jet transverse momenta (HT); or two different types on high-energy particles, such as a muon and an electron and a high scalar sum of the jet transverse momenta (HT) or high missing transverse momentum in the event.
Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.
Data processing / RECO
This primary AOD dataset was processed from the RAW dataset by the following step:
Step: RECO
Release: CMSSW_5_3_7_patch5
Global tag: FT_R_53_V18::All
Configuration file for RECO step reco_2012A_MuHad
HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleDisplacedMu4_DiPFJet40Neutral
HLT_DoubleMu14_Mass8_PFMET40
HLT_DoubleMu14_Mass8_PFMET50
HLT_DoubleMu8_Mass8_PFHT175
HLT_DoubleMu8_Mass8_PFHT225
HLT_DoubleMu8_Mass8_PFNoPUHT175
HLT_DoubleMu8_Mass8_PFNoPUHT225
HLT_DoubleRelIso1p0Mu5_Mass8_PFHT175
HLT_DoubleRelIso1p0Mu5_Mass8_PFHT225
HLT_DoubleRelIso1p0Mu5_Mass8_PFNoPUHT175
HLT_DoubleRelIso1p0Mu5_Mass8_PFNoPUHT225
HLT_IsoMu12_DoubleCentralJet65
HLT_IsoMu12_RsqMR30_Rsq0p04_MR200
HLT_IsoMu12_RsqMR40_Rsq0p04_MR200
HLT_IsoMu17_eta2p1_DiCentralPFJet30_PFHT350_PFMHT40
HLT_IsoMu17_eta2p1_DiCentralPFNoPUJet30_PFNoPUHT350_PFMHT40
HLT_IsoMu17_eta2p1_TriCentralPFJet30
HLT_IsoMu20_eta2p1_CentralPFJet30
HLT_IsoMu20_eta2p1_CentralPFJet30_BTagIPIter
HLT_IsoMu20_eta2p1_CentralPFJet80
HLT_IsoMu20_eta2p1_CentralPFNoPUJet30
HLT_IsoMu20_eta2p1_CentralPFNoPUJet30_BTagIPIter
HLT_IsoMu20_eta2p1_DiCentralPFJet30
HLT_IsoMu20_eta2p1_DiCentralPFNoPUJet30
HLT_IsoMu20_eta2p1_TriCentralPFJet30
HLT_IsoMu20_eta2p1_TriCentralPFJet50_40_30
HLT_IsoMu20_eta2p1_TriCentralPFNoPUJet30
HLT_IsoMu20_eta2p1_TriCentralPFNoPUJet50_40_30
HLT_IsoMu20_eta2p1_WCandPt80
HLT_IsoMu24_eta2p1_CentralPFJet30_CentralPFJet25
HLT_IsoMu24_eta2p1_CentralPFJet30_CentralPFJet25_PFMET20
HLT_IsoMu24_eta2p1_PFJet30_PFJet25_Deta3
HLT_L2TripleMu10_0_0_NoVertex_PFJet40Neutral
HLT_Mu12_DoubleCentralJet65
HLT_Mu12_RsqMR30_Rsq0p04_MR200
HLT_Mu12_RsqMR40_Rsq0p04_MR200
HLT_Mu12_RsqMR45_Rsq0p04_MR200
HLT_Mu12_eta2p1_DiCentral_20
HLT_Mu12_eta2p1_DiCentral_40_20
HLT_Mu12_eta2p1_DiCentral_40_20_BTagIP3D1stTrack
HLT_Mu12_eta2p1_DiCentral_40_20_DiBTagIP3D1stTrack
HLT_Mu12_eta2p1_L1Mu10erJetC12WdEtaPhi1DiJetsC
HLT_Mu14_Ele14_CaloIdT_TrkIdVL_Mass8_PFMET40
HLT_Mu14_Ele14_CaloIdT_TrkIdVL_Mass8_PFMET50
HLT_Mu15_eta2p1_TriCentral_40_20_20
HLT_Mu15_eta2p1_TriCentral_40_20_20_BTagIP3D1stTrack
HLT_Mu15_eta2p1_TriCentral_40_20_20_DiBTagIP3D1stTrack
HLT_Mu20_eta2p1_CentralPFJet30_BTagIPIter
HLT_Mu20_eta2p1_CentralPFNoPUJet30_BTagIPIter
HLT_Mu20_eta2p1_TriCentralPFJet30
HLT_Mu20_eta2p1_TriCentralPFJet50_40_30
HLT_Mu20_eta2p1_TriCentralPFNoPUJet30
HLT_Mu20_eta2p1_TriCentralPFNoPUJet50_40_30
HLT_Mu24_eta2p1_CentralPFJet30_CentralPFJet25
HLT_Mu24_eta2p1_PFJet30_PFJet25_Deta3
HLT_Mu40_FJHT200
HLT_Mu40_HT200
HLT_Mu40_PFHT350
HLT_Mu40_PFNoPUHT350
HLT_Mu60_PFHT350
HLT_Mu60_PFNoPUHT350
HLT_Mu8_DiJet30
HLT_Mu8_Ele8_CaloIdT_TrkIdVL_Mass8_PFHT175
HLT_Mu8_Ele8_CaloIdT_TrkIdVL_Mass8_PFHT225
HLT_Mu8_Ele8_CaloIdT_TrkIdVL_Mass8_PFNoPUHT175
HLT_Mu8_Ele8_CaloIdT_TrkIdVL_Mass8_PFNoPUHT225
HLT_Mu8_QuadJet30
HLT_Mu8_TriJet30
HLT_PFHT350_Mu15_PFMET45
HLT_PFHT350_Mu15_PFMET50
HLT_PFHT400_Mu5_PFMET45
HLT_PFHT400_Mu5_PFMET50
HLT_PFNoPUHT350_Mu15_PFMET45
HLT_PFNoPUHT350_Mu15_PFMET50
HLT_PFNoPUHT400_Mu5_PFMET45
HLT_PFNoPUHT400_Mu5_PFMET50
HLT_RelIso1p0Mu5_Ele8_CaloIdT_TrkIdVL_Mass8_PFHT175
HLT_RelIso1p0Mu5_Ele8_CaloIdT_TrkIdVL_Mass8_PFHT225
HLT_RelIso1p0Mu5_Ele8_CaloIdT_TrkIdVL_Mass8_PFNoPUHT175
HLT_RelIso1p0Mu5_Ele8_CaloIdT_TrkIdVL_Mass8_PFNoPUHT225
During data taking all the runs recorded by CMS are certified as good for physics analysis if all subdetectors, trigger, lumi and physics objects (tracking, electron, muon, photon, jet and MET) show the expected performance. Certification is based first on the offline shifters evaluation and later on the feedback provided by detector and Physics Object Group experts. Based on the above information, which is stored in a specific database called Run Registry, the Data Quality Monitoring group verifies the consistency of the certification and prepares a json file of certified runs to be used for physics analysis. For each reprocessing of the raw data, the above mentioned steps are repeated. For more information see:
CMS data quality monitoring: Systems and experiences
The CMS Data Quality Monitoring software experience and future improvements
The CMS data quality monitoring software: experience and future prospects
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