4l analysis with pf2pat

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4l analysis with PF2PAT June 6, 2012 Jongseok Lee (Sungkyunkwan University) 1

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4l analysis with PF2PAT. June 6, 2012 Jongseok Lee (Sungkyunkwan University). Used samples. /TTTo2L2Nu2B_7TeV-powheg-pythia6/jslee-v2-Fall11_TTTo2L2Nu2B-f99e9bb67aff534e9b6be7177a9a6dd1/USER - PowerPoint PPT Presentation

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Page 1: 4l analysis with PF2PAT

4l analysis with PF2PAT

June 6, 2012 Jongseok Lee(Sungkyunkwan University)

1

Page 2: 4l analysis with PF2PAT

Used samples/TTTo2L2Nu2B_7TeV-powheg-pythia6/jslee-v2-Fall11_TTTo2L2Nu2B-f99e9bb67aff534e9b6be7177a9a6dd1/USER/DYJetsToLL_TuneZ2_M-50_7TeV-madgraph-tauola/jslee-v2-Fall11_DYJetsToLL_M-50-f99e9bb67aff534e9b6be7177a9a6dd1/USER/DYJetsToLL_M-10To50_TuneZ2_7TeV-madgraph/jslee-v2-Fall11_DYJetsToLL_M-10To50-f99e9bb67aff534e9b6be7177a9a6dd1/USER/ZZJetsTo2L2Q_TuneZ2_7TeV-madgraph-tauola/jslee-v2-Fall11_ZZJetsTo2L2Q-f99e9bb67aff534e9b6be7177a9a6dd1/USER/ZZJetsTo2L2Nu_TuneZ2_7TeV-madgraph-tauola/jslee-v2-Fall11_ZZJetsTo2L2Nu-f99e9bb67aff534e9b6be7177a9a6dd1/USER/ZZJetsTo4L_TuneZ2_7TeV-madgraph-tauola/jslee-v2-Fall11_ZZJetsTo4L-f99e9bb67aff534e9b6be7177a9a6dd1/USER/WZJetsTo3LNu_TuneZ2_7TeV-madgraph-tauola/jslee-v2-Fall11_WZJetsTo3LNu-f99e9bb67aff534e9b6be7177a9a6dd1/USER/WWJetsTo2L2Nu_TuneZ2_7TeV-madgraph-tauola/jslee-v2-Fall11_WWJetsTo2L2Nu-f99e9bb67aff534e9b6be7177a9a6dd1/USER/T_TuneZ2_tW-channel-DR_7TeV-powheg-tauola/jslee-v2-Fall11_T_tW-channel-f99e9bb67aff534e9b6be7177a9a6dd1/USER/T_TuneZ2_t-channel_7TeV-powheg-tauola/jslee-v2-Fall11_T_t-channel-f99e9bb67aff534e9b6be7177a9a6dd1/USER/T_TuneZ2_s-channel_7TeV-powheg-tauola/jslee-v2-Fall11_T_s-channel-f99e9bb67aff534e9b6be7177a9a6dd1/USER/Tbar_TuneZ2_tW-channel-DR_7TeV-powheg-tauola/jslee-v2-Fall11_Tbar_tW-channel-f99e9bb67aff534e9b6be7177a9a6dd1/USER/Tbar_TuneZ2_t-channel_7TeV-powheg-tauola/jslee-v2-Fall11_Tbar_t-channel-f99e9bb67aff534e9b6be7177a9a6dd1/USER/Tbar_TuneZ2_s-channel_7TeV-powheg-tauola/jslee-v2-Fall11_Tbar_s-channel-f99e9bb67aff534e9b6be7177a9a6dd1/USER

/DoubleMu/jslee-v1-Fall11_DoubleMu_Run2011A_05Aug2011_v1-964e7d21029af38f9c00329957b4d353/USER/DoubleMu/jslee-v1-Fall11_DoubleMu_Run2011A_May10ReReco_v1-d31f607963c7fe80e3344181c12a0e60/USER/DoubleMu/jslee-v1-Fall11_DoubleMu_Run2011A_PromptReco_v4-964e7d21029af38f9c00329957b4d353/USER/DoubleMu/jslee-v1-Fall11_DoubleMu_Run2011A_PromptReco_v6-037418361e29e96631af775307e2c915/USER/DoubleMu/jslee-v1-Fall11_DoubleMu_Run2011B_PromptReco_v1-037418361e29e96631af775307e2c915/USER

/DoubleElectron/jslee-v1-Fall11_DoubleElectron_Run2011A_05Aug2011_v1-7d72a8e72006e808591999f6bafa3866/USER/DoubleElectron/jslee-v1-Fall11_DoubleElectron_Run2011A_May10ReReco_v1-3b82207fc35d51fff8d7425676ffcb81/USER/DoubleElectron/jslee-v1-Fall11_DoubleElectron_Run2011A_PromptReco_v4-5985f686a9776bffdb56ca6460a22c2f/USER/DoubleElectron/jslee-v1-Fall11_DoubleElectron_Run2011A_PromptReco_v6-15a0cdac6fbf3d95ed3e755903591ee3/USER/DoubleElectron/jslee-v1-Fall11_DoubleElectron_Run2011B_PromptReco_v1-15a0cdac6fbf3d95ed3e755903591ee3/USER

/MuEG/seungen-v1-Fall11_MuEG_Run2011A_May10ReReco_v1-60bef32a1967e0b919dbf9da747a1044/USER/MuEG/seungen-v1-Fall11_MuEG_Run2011A_PromptReco_v4-4545b3facad91df4dfb06138bbc7587c/USER/MuEG/seungen-v1-Fall11_MuEG_Run2011A_PromptReco_v6-c8990932f52e017973bc54739a51f06e/USER/MuEG/seungen-v1-Fall11_MuEG_Run2011A_05Aug2011_v1-1aab3f74f26f9522ea3482d1757b6789/USER/MuEG/seungen-v1-Fall11_MuEG_Run2011B_PromptReco_v1-c8990932f52e017973bc54739a51f06e/USER 2

Page 3: 4l analysis with PF2PAT

HLT & skim efficiency

3

HLT eff = Nhlt/Ngen, Skim eff = Nskim/Nhlt

Page 4: 4l analysis with PF2PAT

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HLT & skim efficiency HLT eff = Nhlt/Ngen, Skim eff = Nskim/Nhlt

Page 5: 4l analysis with PF2PAT

Lepton & event selection

5

• Electron selection pT>10 GeV, |η|<2.5, |d0|<0.02, sip<4, nchi2<10, charge consistent, eidLoose

• Muon selectionpT>10 GeV, |η|<2.4, global muon, good muon, nchi2<10, hits_val>20, nstation>=1

• Preselection : nlep+>=2, nlep->=2

• Event selection - mass dependent cut

m4 cut : |mp – mn|/(mp + mn) > cut value

di-lepton pt cut : Max(pT(H++),pT(H--),pT(Z1),pT(Z2)) > cut value

Page 6: 4l analysis with PF2PAT

6

m4 for event selection

GeV

exp

ect

ed

# o

f even

t

nlep+>=2, nlep->=2

exp

ect

ed

# o

f even

t

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

H++H– to eeee(130GeV)

H++H-- to eeee(200GeV)

H++H-- to μμμμ(130GeV)

H++H-- to eμeμ(130GeV)

GeV

GeV

GeV

GeV

GeV

H++H-- to μμμμ(200GeV)

H++H-- to eμeμ(130GeV)

Page 7: 4l analysis with PF2PAT

7

dilpt for event selection

GeV

exp

ect

ed

# o

f even

t

nlep+>=2, nlep->=2, m4

exp

ect

ed

# o

f even

t

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

H++H– to eeee(130GeV)

H++H-- to eeee(200GeV)

H++H-- to μμμμ(130GeV)

H++H-- to eμeμ(130GeV)

GeV

GeV

GeV

GeV

GeV

H++H-- to μμμμ(200GeV)

H++H-- to eμeμ(200GeV)

Page 8: 4l analysis with PF2PAT

Mass of H++

8GeV

nlep+>=2, nlep->=2

GeV

GeV

GeV

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

H++H– to eeee(130GeV)

H++H-- to eeee(200GeV)

H++H-- to μμμμ(130GeV)

H++H-- to eμeμ(130GeV)

GeV

GeV

GeV

GeV

GeV

H++H-- to μμμμ(200GeV)

H++H-- to eμeμ(200GeV)

Page 9: 4l analysis with PF2PAT

Mass of H++

9GeV

nlep+>=2, nlep->=2, m4

GeV

GeV

GeV

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

exp

ect

ed

# o

f even

texp

ect

ed

# o

f even

t

H++H– to eeee(130GeV)

H++H-- to eeee(200GeV)

H++H-- to μμμμ(130GeV)

H++H-- to eμeμ(130GeV)

GeV

GeV

GeV

GeV

GeV

H++H-- to μμμμ(200GeV)

H++H-- to eμeμ(200GeV)

Page 10: 4l analysis with PF2PAT

Exclusion limit

10

nlep+>=2, nlep->=2, m4, dilpt

ememExpected Limit : 360 GeVObserved Limit : 362 GeV

eeeeExpected Limit : 348 GeVObserved Limit : 349 GeV

mmmmExpected Limit : 379 GeVObserved Limit : 380 GeV

Page 11: 4l analysis with PF2PAT

Weekly plan

• Delta-beta correction for particle flow isolation

11

Page 12: 4l analysis with PF2PAT

backup

12

Page 13: 4l analysis with PF2PAT

Mario’s result with Fall11

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Combined Limit : 459 GeV // Limit for pair production only 392 GeV