search of the higgs boson in the ww (*) decay channel with the cms experiment
DESCRIPTION
Search of the Higgs boson in the WW (*) decay channel with the CMS experiment. We are ready to go !. Lake Louise Winter Institute. Ezio Torassa - INFN Padova. 18 th - 23 th February 2008 Alberta , Canada. On behalf of the CMS collaboration. Higgs production at the LHC. - PowerPoint PPT PresentationTRANSCRIPT
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Search of the Higgs Search of the Higgs boson in the WW boson in the WW (*)(*)
decay channel with the decay channel with the CMS experiment CMS experiment
We are ready to go !
18th - 23th February 2008 Alberta , Canada
Lake Louise Winter Lake Louise Winter Institute Institute
On behalf of the CMS collaboration
Ezio Torassa - INFN Ezio Torassa - INFN PadovaPadova
Lake Louise – February 2008 Ezio Torassa – INFN Padova 2
CMS Physics TDR Vol 2
Higgs production at the LHC
SM Higgs production cross section including NLO QCD corrections
Lake Louise – February 2008 Ezio Torassa – INFN Padova 3
Higgs branching ratios
The Higgs coupling constants to fermions and bosons are proportional to the particle masses:
For Higgs masses above 135 GeV the main decay modes are those
into WW(*) and ZZ(*)
(under 135 GeV b/c quarks and +-)
ff
fhfm
v
mg
WV
hVV Mv
mg
22
2GeV/c246sin
WWMv
CMS Physics TDR Vol 2
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Signal and Backgrounds
Continuum production of WW pairs
Wt
The signal is characterized by:
- two high Pt isolated leptons - missing Et- no high energy Jet - angle correlation between WW
DYtt
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Monte Carlo simulation
Higgs boson signal samples were generated using the LO PHYTIA Monte Carlo.The events were reweighted to match expectation from NLO. k(pT) factors were calculated with the MC@NLO Monte Carlo.
))((p
))((p
T
T
PYTHIALO
orderhigher)(pTk
The total NLO cross section is rescaled considering NLO calculations.The same procedure was used for the dominant irreducible WW background.
For the other backgrounds the inclusive k factor was used:
tt and Wt were produced using the TopRex Monte Carlo
kinc = ∫ k(pT) dpT
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The CMS recent H→WW analysis
Standard Model Higgs Discovery Potential of CMS NOTE 2006/047CMS in the H→WW→ll channel
Systematic uncertainties of the top background CMS NOTE 2006/048In the H→WW channel
Physics study of the Higgs decay channel CMS NOTE 2006/055 H→WW(*)→22
Search for a Light Standard Model Higgs boson CMS NOTE 2006/114in the H→WW(*)→eechannel
Search for the Higgs boson in the WW(*) decay CMS PAS Hig_07_001Channel with the CMS experiment
CMS TDR vol II Cut based
CMS PAS Hig_07_001 Cut based + TMVA
Summary inside
CMS TDR vol II
Physics Performance
This report =>
Low Higgs Mass
optimization
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H→WW analysis CMS PTDR vol. II
MET Ptmax
Ptmin
Isolation
IP < 3 for each muon
Jet Veto
Missing ET > 50 GeV
55 GeV > ptmax > 35 GeV
ptmin > 25 GeV
Inv. Mass < 50 GeV
between muons < 0.8
Inv. Mass
( L = 10 fb-1 )
The selection tools ( channel )
tt WW DY
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H→WW analysis CMS PTDR vol. II
Angle between the leptons
Final selection + e + ee channels
l = e , , NLO x BR (pb) Rate / fb-1
H→WW→ll (160 GeV) 2.34 42
H→WW→ll (165 GeV) 2.36 46
H→WW→ll (170 GeV) 2.26 33
qq→WW→ll 11.7 12
gg→WW→ll 0.48 3.7
tt→WWbb→ll 86.2 9.8
tW→WWb→ll 3.4 1.4
ZW→lll 1.6 0.5
ZZ→ll 1.5 0.35
Sum backgrounds 105 28
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control region signal region
H→WW analysis CMS PTDR vol. II
regcontrolMCregcontrol
MCregsignal
regsignal NN
NN _
_
__
JET veto removed
2 b-tagged jets
Background estimation from data
H→WW
tt
WW
control region
tt
tt
Systematic error estimation
Th. err. Det. sys. Stat. err.
Tot. errors @ L = 5 fb-1 16% 17%
regcontrolMCregcontrol
MCregsignal
MCregcontrol
MCregsignal
regcontrolMCregcontrol
MCregsignal
regsignal NNN
NN _
_
_
_
__
_
__
tt
tt WW
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H→WW analysis CMS PTDR vol. II
Signal significance Luminosity for discovery at 5
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H→WW analysis CMS PAS Hig_07_001
trigger + skim pre-selectionmultivariate
analysis
cut based analysis
Analysis strategy
one pair of leptons with opposite charge |η1| < 2.5, |η2| < 2.5 MET > 30 GeV m(ll) >= 12 GeV Njets central <= 2 (ET > 20 GeV)
ptmin > 10 GeV, ptmax
> 20 GeV
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H→WW analysis CMS PAS Hig_07_001
Analysis strategy
- mass dependent cuts optimization- optimized significance defined as:
nσ (cuts) = NS / √[NB + (ΔNB)2]
- test of different Multivariate Techniques: boosted decision tree (BDT) neural network classifiers (NN)
Classifier output for the boosted decision tree analysis
Cut based analysis
Multivariate analysis
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Conclusions
The Monte Carlo analysis preformed for the PTDR vol. II showed the SM Higgs boson could be discovered with: - less than 1 fb-1 if its mass is around 165 GeV - 10 fb-1 if its mass is between 150 GeV and 180 GeV
More detailed studies are showing that we can increase the sensibility in the low mass region with: - mass dependent cut based analysis - multivariate analysis techniques
Next results will provide exclusion limits with the 100 pb-1
misalignment scenario