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ttH can be feasible using ttH can be feasible using shape ….?shape ….?
Samir FERRAGSamir FERRAG
University of GlasgowUniversity of Glasgow Les Houches, 23/06/2007Les Houches, 23/06/2007
Not Official ATLAS results
HHbb, via ttH with mH< 130 GeVbb, via ttH with mH< 130 GeV• Complex and challenging channel (HComplex and challenging channel (Hbb):bb):
– One lepton (trigger)One lepton (trigger)– 4 b-jets + 2 jets4 b-jets + 2 jets
Need excellent b-tagging: Need excellent b-tagging: signal efficiency ~O(signal efficiency ~O(44bb))
– Fully reconstructed tFully reconstructed t– High jet multiplicity High jet multiplicity
• CombinatoricsCombinatorics• Difficult to simulateDifficult to simulate
• Background:Background:– Reducible: tt+jj, W+jets, WWbbjjReducible: tt+jj, W+jets, WWbbjj
• Extracted from dataExtracted from data• Reduced by imposing reconstructed tt pair Reduced by imposing reconstructed tt pair
– Irreducible: ttbb, combinatoricsIrreducible: ttbb, combinatorics• Slight difference in kinematics with the signal (Likelihood)Slight difference in kinematics with the signal (Likelihood)
Evolution of resultsEvolution of results• After an optimistic evaluation on
the TDR:– Updating pdf: 20% smaller cross sections– Matrix element based Monte Carlo for ttbb
background higher jet multiplicity
• Realistic environment– Significance down to < 2
Counting experiment:Counting experiment:
Constraints on the ttH analysisConstraints on the ttH analysis • Higgs mass=120GeV• Higgs mass=130GeV
• 10 fb-1
• 100 fb-1
ATLFASTanalysis
ATLFASTanalysis
The constraints on ttH are challenging
CE: Constraint on ttH for 10fbCE: Constraint on ttH for 10fb-1-1
5
4
3
2
6% of PDF uncertainties (on ttbb+ttjj)
S/B
systematic uncertainty on B (%)
Requested S/BFor 3 significaneFor 6% PDF uncertainty
Need 1 to 2 % of accuracyOn background to reach 2 significance
• Higgs mass=120GeV
S/B=0.14 From Markus analysis(ATLFAST)
Signal ReconstructionSignal Reconstruction
The signal is plagued by wrong combinatorial pairs (>70%) which makes it looking-like the background --> - lower the S/B power
Signal Background
Wright combinations
Likelihood2 for the Signal/BackgroundLikelihood2 for the Signal/Background
Robustness of distributions validated by a comparison between MC@NLO and ACERMC
Likelihood1 to reduce combinatoricsLikelihood1 to reduce combinatorics
CE: Sensitivity results CE: Sensitivity results (without systematics)(without systematics)
Current Analyses:
A1- Cuts Based Analysis: C. Collins-Tooth s/b=1.9
A2- Selected Likelihood: G. Aad s/b=3.1
90 -150 GeV
s/b is computed in thisInterval (Signal Interval)
– For 100fb-1 (in 2011) and Background accuracy of 5%5% :• S/B=30% for a 5 discovery (mHiggs=120 GeV)
• S/B=16% for a 3 evidence (mHiggs=120 GeV)
Shape Analysis: Getting and using Shape Analysis: Getting and using 22
H0
H0 ---> t0 ( where t0 is a template for the null hypothesis, H0. )
• H1 ---> t1 ( where t1 is a template for the signal plus background hypothesis, H1. )
• ‘Data’ ---> gives us one 02 (H0) and 1
2 (H1).
• Generate ‘Data’ 10000 times (in pseudo experiments).
2lnQ =-2
H1
2 = 9.876e.g.
• 1 - CLb = Probability that the background will fluctuate to look like the signal
Equivalent in counting experiment: …….5 1-CLb = 2x10-7.
•CLs+b = Confidence Level for excluding H0.
Use:-
CLs+b 1 - CLb
Improvement from using shapeImprovement from using shape
Shape Analysis 2
(CE) One Bin 2
H1H0
Effect of shapesEffect of shapes
Probability of measuring with 30fb-1
3 5
Counting Experiment 19% <1%
Shape 38% 3%
Shape 15% on Signal X-sec
30% 1%
Probability of measuring with 30fb-1 2 3
Counting Experiment 30% 6%
Shape 34% 8%
Cut based analysis
Likelihood analysis
The hape of distributions helps for both likelihood and shape analysis but is it robust?
Backup slides
CE: Constraint on ttH for 100fbCE: Constraint on ttH for 100fb-1-1
6% of PDF uncertainties
S/B
systematic uncertainty on B (%)
Requested S/BFor 3 significaneFor 6% PDF uncertainty
5
4
3
2
Need 4% of accuracyOn background to reach 3 significance
S/B=0.14 From Markus analysis(ATLFAST)
• Higgs mass=120GeV