higgs search in the h➝bb channel in atlas
DESCRIPTION
Higgs search in the H➝bb channel in ATLAS. Ricardo Gonçalo Royal Holloway University of London on behalf of the ATLAS Collaboration. International Europhysics Conference on High Energy Physics, Grenoble, July 21-27 2011. Outline. ATLAS and the LHC Higgs physics at the LHC - PowerPoint PPT PresentationTRANSCRIPT
H->+- and H+-> with the ATLAS Detector at the LHC
Higgs search in the Hbb channel in ATLASRicardo Gonalo Royal Holloway University of Londonon behalf of the ATLAS Collaboration
International Europhysics Conference on High Energy Physics, Grenoble, July 21-27 2011OutlineATLAS and the LHC
Higgs physics at the LHC
ZH/WH Hbb in ATLASEvent selectionBackgroundsSystematic errorsResults
Boosted VH
Summary and OutlookRicardo GonaloEPS-HEP 2011 - Grenoble - July 20112
ATLAS and the LHCRicardo GonaloEPS-HEP 2011 - Grenoble - July 20113Ricardo GonaloEPS-HEP 2011 - Grenoble - July 20114
JINST (2008) 3 S08003Inner Tracker: ||20GeV) or (pT>18GeV)Exactly 1 lepton pT > 25GeVMT = 2pTlpT(1 - cos l ) > 40 GeVETmiss > 25GeV Exactly 2 jets (anti-kT 0.4; ET > 25GeV) to reduce top backgroundBoth jets b taggedRicardo GonaloEPS-HEP 2011 - Grenoble - July 201113To be included if approvedTo be included if approvedTo be included if approvedWHlbb BackgroundsW+jets and top dominant:W+jets important at low mbb:Use mjj from data as templateTop dominant at high mbb:Describe shape with MCCross check mbb in 3-jet binNormalisation from mbb sidebands [40GeV, 80 GeV] and [140GeV, 250GeV] Z+jets: use same normalisation of MC as measured in ZHMultijet Data templates from QCD enhanced samples (anti-isolation)Diboson WW , WZ from Monte CarloRicardo GonaloEPS-HEP 2011 - Grenoble - July 201114To be included if approvedTo be included if approved
Dominant systematic errors from b-tagging efficiency in both analyses
Followed by jet energy scale
Points at the next things things to improve!
Ricardo GonaloEPS-HEP 2011 - Grenoble - July 201115Size of Systematic UncertaintiesZHllbb WHlbb To be included if approvedTo be included if approvedHbb Analysis ResultsRicardo GonaloEPS-HEP 2011 - Grenoble - July 201116ZHllbb Good description of the backgroundNo excess observedSingle-channel exclusion of 20x Standard ModelRicardo GonaloEPS-HEP 2011 - Grenoble - July 201117To be included if approvedTo be included if approvedTo be included if approved
WHlbb Good description of the backgroundNo excess observedSingle-channel exclusion of 20-30x Standard ModelRicardo GonaloEPS-HEP 2011 - Grenoble - July 201118To be included if approvedTo be included if approvedTo be included if approved
Boosted VH with HbbRicardo GonaloEPS-HEP 2011 - Grenoble - July 201119Select Wl events and search for a Hbb jet Search for high-pT jet (Cambridge-Aachen algorithm, R=1.2)Search jet clustering history in reverse and look for large mass dropRe-cluster with small R parameter to find sub jets
Peak consistent with Wjj in tt events Proof of principle for future analysisAlternative to inclusive channels: search for high-pT Higgs to bb: J. M. Butterworth, A. R. Davison, M. Rubin, and G. P. Salam, Phys. Rev. Lett. 100 (2008) 242001, arXiv:0802.2470 [hep-ph]pTH > 200GeV 5% of inclusive cross section but improved significanceRicardo Gonalo20
To be included if approvedConclusions & OutlookRicardo GonaloEPS-HEP 2011 - Grenoble - July 201121First direct search for Hbb at the LHC in WH and ZH channels
Room for improvement! Reduce systematicsNew channels to exploreMultivariate analysesLots of data expected!
Proof of principle for boosted Higgs analysis
Watch this space! Ricardo GonaloEPS-HEP 2011 - Grenoble - July 201122To be included if approvedTo be included if approvedBackupRicardo GonaloEPS-HEP 2011 - Grenoble - July 201123ATLAS & LHC: Efficiency and PileupVery good ATLAS performanceData-taking efficiency above 95%Luminosity-weighted distribution of the mean number of interactions per crossing for 2011Calculated from the instantaneous luminosity as: =L x inel / (nbunch x fr) L: instantaneous luminosityinel : inelastic cross section (71.5 mb)nbunch: number of colliding bunchesfr: LHC revolution frequencyEntries at 0 from pilot bunches See: arXiv:1101.2185
Ricardo GonaloEPS-HEP 2011 - Grenoble - July 201124
Monte Carlo SamplesaRicardo GonaloEPS-HEP 2011 - Grenoble - July 201125
Common event selection:
Lepton Identification:
Jet reconstruction:Ricardo GonaloEPS-HEP 2011 - Grenoble - July 201126
Detector related uncertaintiesRicardo GonaloEPS-HEP 2011 - Grenoble - July 201127
Normalization Systematic UncertaintiesRicardo GonaloEPS-HEP 2011 - Grenoble - July 201128
Guessing the Tevatron sensitivityProbably close to excluding (or not) the Higgs at low massAt 4x SM with ZH->bb last yearSeveral factors 2x wrt now: 2 experimentsadding lepton channelsincreased luminosityRicardo GonaloEPS-HEP 2011 - Grenoble - July 201129NOT to show at conferencehttp://tevnphwg.fnal.gov/July 2010http://tevnphwg.fnal.gov/March 2011ZH->bb; March 2011On high-pT jet massCut applied here at 300GeV gives peak at 50-100Partially removed by jet filtering but shoulder still visible in boosted W->jj plotRicardo GonaloEPS-HEP 2011 - Grenoble - July 201130
NOT to show at conference
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LHC DeliveredATLAS Recorded
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-1 s-2 cm33 10Peak Lumi: 1.26
110
100 110 120 130 140 150 160 170 180 190 200
1
10
mH(GeV/c2)
95%
CL
Limi
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Tevatron Run II Preliminary, = 5.9 fb-1
ExpectedObserved1m Expected2m Expected
LEP Exclusion TevatronExclusion
SM=1
Tevatron Exclusion July 19, 2010
110
130 140 150 160 170 180 190 200
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10
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95%
CL L
imit/S
MTevatron Run II Preliminary, L ) 8.2 fb-1
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TevatronExclusion
SM=1
March 7, 2011
[GeV] m60 70 80 90 100 110 120 130 140 150
Entri
es /
3 Ge
V
1
10
210
310
410
510
610 dataTotal MCZTopDibosonMultijetW
ATLAS Preliminary-1 L dt=1.04 fb0 muon channel
[GeV]missT E0 50 100 150 200
Entri
es /
4 Ge
V
-210
-1101
10210
310
410
510
610 dataTotal MCZTopDibosonMultijetW
ATLAS Preliminary-1 L dt=1.04 fb0
b-Jet N0 1 2 3
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110
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710 dataTotal MCZTopDibosonMultijetW
ATLAS Preliminary-1 L dt=1.04 fb0
[GeV] bb m0 50 100 150 200 250
Ent
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02468
101214161820
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ATLAS Preliminary-1 L dt=1.04 fb0
[GeV] bj m0 50 100 150 200 250
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GeV
050
100150200250300350
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100150200250300350 data
Total MCZOther BG
ATLAS Preliminary-1 L dt=1.04 fb0
[GeV]iT e m0 20 40 60 80 100 120 140
Entri
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10
210
310
410
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610 data Total MCW TopDiboson Multijet
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data Total MCW TopDiboson Multijet
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ATLAS Preliminary-1 L dt=1.04 fb0
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210
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610
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ATLAS Preliminary-1 L dt=1.04 fb0
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610dataTotal MCWTopDibosonMultijetZ
ATLAS Preliminary-1 L dt=1.04 fb0
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[GeV]bb m0 50 100 150 200 250
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[GeV]bb m0 50 100 150 200 250
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020406080
100120140160180200220 data
20Signal =130 GeV)
H(mTotal BGZWTopDibosonMultijet
ATLAS Preliminary-1 L dt=1.04 fb0
[GeV] bb m0 50 100 150 200 250
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ries /
10
GeV
050
100150200250300350400
[GeV] bb m0 50 100 150 200 250
Ent
ries /
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GeV
050
100150200250300350400
dataTotal MCTopOther BG
ATLAS Preliminary-1 L dt=1.04 fb0
Higgs mass [GeV]110 115 120 125 130
SMm/m
95%
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20
40
60
80
100
120 Observed (CLs)Expected (CLs)m 1m 2 bbAZH, H
ATLAS Preliminary
=7 TeVs, -1 Ldt=1.04 fb0
[GeV]bb m0 50 100 150 200 250
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GeV
05
1015202530354045
[GeV]bb m0 50 100 150 200 250
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1015202530354045 data
20Signal =115 GeV)
H(mTotal BGZTopDiboson
ATLAS Preliminary-1 L dt=1.04 fb0
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1015202530354045 data
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1015202530354045 data
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[GeV]bb m0 50 100 150 200 250
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GeV
05
1015202530354045 data
20Signal =130 GeV)
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ATLAS Preliminary-1 L dt=1.04 fb0
[GeV]bb m0 50 100 150 200 250
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10
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020406080
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[GeV]bb m0 50 100 150 200 250
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[GeV]bb m0 50 100 150 200 250
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10
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100120140160180200220 data
20Signal =130 GeV)
H(mTotal BGZWTopDibosonMultijet
ATLAS Preliminary-1 L dt=1.04 fb0
Higgs mass [GeV]110 115 120 125 130
SMm/m
95%
C.L
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20
40
60
80
100
120 Observed (CLs)Expected (CLs)m 1m 2 bbAWH, H
ATLAS Preliminary
=7 TeVs, -1 Ldt=1.04 fb0
[GeV]bb m0 50 100 150 200 250
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020406080
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100 110 120 130 140 150 160 170 180 190 200
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Tevatron Run II Preliminary, = 5.9 fb-1
ExpectedObserved1m Expected2m Expected
LEP Exclusion TevatronExclusion
SM=1
Tevatron Exclusion July 19, 2010
110
130 140 150 160 170 180 190 200
1
10
mH (GeV/c2)
95%
CL L
imit/S
MTevatron Run II Preliminary, L ) 8.2 fb-1
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March 7, 2011