scott mcgarvie determining the cp properties of a light higgs boson
DESCRIPTION
Scott McGarvie Determining the CP Properties of a Light Higgs Boson. Royal Holloway, University of London. Contents. Introduction Heavy Higgs CP Light Higgs CP Production/Decay Channel Selection procedure CP sensitive variables Conclusions and Future Plans. Introduction - PowerPoint PPT PresentationTRANSCRIPT
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Scott McGarvie Atlas UK, 15/12/03
Scott McGarvie
Determining the CP Properties of a Light Higgs Boson
Royal Holloway, University of London
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Scott McGarvie Atlas UK, 15/12/03
•Introduction
•Heavy Higgs CP
•Light Higgs CP
•Production/Decay Channel
•Selection procedure
•CP sensitive variables
•Conclusions and Future Plans
Contents
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Scott McGarvie Atlas UK, 15/12/03
IntroductionThe search for the Higgs boson is one of the most important tasks for the LHC
Demonstrated for the TDR that ATLAS can cover the whole SM parameter space
Once the Higgs is discovered, we will need to study its properties
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Scott McGarvie Atlas UK, 15/12/03
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Scott McGarvie Atlas UK, 15/12/03
SM Higgs is spin 0 and CP-even
This may not be the case in models with extended Higgs sectors:
• general 2HDM
•MSSM with complex parameters
Carena, Ellis, Mrenna, Pilaftsis, Wagner. Nucl.Phys. B659 (2003)
145-178 - hep-ph/0211467
MSSM predicts 3 neutral Higgs particles. h, H (CP-even) A (CP-odd)Presence of complex phases causes mixing and the mass eigenstates (h1, h2, h3) then have mixed CP
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Scott McGarvie Atlas UK, 15/12/03
Experimental evidence that demonstrates the CP quantum numbers, would be very useful in determining the correct model
Making a precision measurement such as this will be very difficult in the messy environment of the LHC
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Scott McGarvie Atlas UK, 15/12/03
Heavy Higgs CP
•CP even parallel decay planes,
•CP odd perpendicular
Buszello, Fleck, Marquard, Van der Bij, SN-ATLAS-2003-025
CP Information is contained in the decay planes of H → ZZ* → 4l
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Scott McGarvie Atlas UK, 15/12/03
It was shown that they can distinguish between a CP-even and a CP-odd with 100fb-1, for a Higgs mass 200 GeV
The linear collider uses a similar technique to determine the CP
Running in the mode, the polarisation of the photons can be changed from parallel to perpendicular to preferentially produce either a CP-even or CP-odd state
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Scott McGarvie Atlas UK, 15/12/03
Higgs Decays
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Scott McGarvie Atlas UK, 15/12/03
Higgs production
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Scott McGarvie Atlas UK, 15/12/03
Interaction Lagrangian
Light Higgs CP
2 2 2 2M ( )QM c d
For a light Higgs the H → ZZ* branching fraction is too small
Use H → bb, , + decay channels
c is the CP-even coupling and d is the CP-odd coupling
SM has c = 1 and d = 0
Using ideas from Gunion, He PRL 76, 24, 4468 (1996)
Only top quark will have significant sensitivity to CP
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Scott McGarvie Atlas UK, 15/12/03
CP sensitive variables
CP information contained in the momenta of the tops
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Scott McGarvie Atlas UK, 15/12/03
Aims
•Use the associated ttH → channel
•Select events with required topology
•Reconstruct the physics objects
•Select events using a 2 technique, to reduce the combinatorial background
•Demonstrate that the CP information is contained with the proposed variables
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Scott McGarvie Atlas UK, 15/12/03
Comment
•Very small event rate
•In the context of the MSSM, the HVV coupling is absent
The ttH → will probably not be the best channel in which to measure CP
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Scott McGarvie Atlas UK, 15/12/03
Comment II
the ttH → bb, +- channels have advantages and disadvantages.
,
Couplings
Branching fractions increase
production cross-section decreases
Much higher signal rate, much higher backgrounds
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Scott McGarvie Atlas UK, 15/12/03
Selection Procedure
•2 or more light jets
•2 bjets
•2 photons (pT 25 GeV)
•1 electron or 1 muon ( pT 25 GeV)
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Scott McGarvie Atlas UK, 15/12/03
Selection efficiencies
For the selected events
•Reconstruct a hadronic W from all jet-jet pairs
•Assume missing momentum is due to the neutrino, use W mass constraint to fully reconstruct the neutrino momentum.
•Reconstruct a leptonic W in events which have 1 or more neutrino solutions
•Reconstruct the top quark by combining the b-jet and W 4-vectors
Cut Nbjet =2 Nljet 2 1e or 1 n 2 pT 25 , e,
1 soln.
CP even (%) 19.4 19.1 6.2 4.9 2.9 2.0
CP odd (%) 19.3 19.2 6.2 5.3 3.8 2.5
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Scott McGarvie Atlas UK, 15/12/03
Hadronic W mass from all jj pairs
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Scott McGarvie Atlas UK, 15/12/03
Hadronic top mass from all bjj
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Scott McGarvie Atlas UK, 15/12/03
Top Reconstruction
4-vectors of the two tops are found by selecting the combination which minimizes the 2
The selected tops are then used to Determine to values of the CP sensitive variables
Reconstruct a top for all bjj and bl combinations.
mt = 175 GeV, mw = 80 GeV, from TDR
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Scott McGarvie Atlas UK, 15/12/03
Reconstructed hadronic W
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Scott McGarvie Atlas UK, 15/12/03
Reconstructed hadronic top
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Scott McGarvie Atlas UK, 15/12/03
Reconstructed semi-leptonic top
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Scott McGarvie Atlas UK, 15/12/03
CP sensitive variables: a1, a2
CP odd
CP evenCP even
CP odd
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Scott McGarvie Atlas UK, 15/12/03
CP sensitive variables: b1, b2
CP odd
CP even
CP even
CP odd
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Scott McGarvie Atlas UK, 15/12/03
CP sensitive variables: b3, b4
CP odd
CP evenCP even
CP odd
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Scott McGarvie Atlas UK, 15/12/03
Future PlansSeveral things still to do
•Finish the semi-leptonic ttH → channel and obtain significances for distinguishing between CP-even and CP-odd
•Backgrounds
•Better operators with greater sensitivity to CP
•Sensitivity to a Higgs with mixed CP
•Other Decay channels
• ttH → , both tops hadronic
• ttH →bb
• ttH →+-
•Combined analysis of different channels
•MC@NLO
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Scott McGarvie Atlas UK, 15/12/03
Conclusions
ATLAS does have some sensitivity to the CP properties of a light higgs.
A precision measurement like this needs high statistics, and may require a combined ATLAS/CMS analysis