Transcript Slide 1

On the Trail of the Higgs Boson
Meenakshi Narain
Outline
• Higgs Primer
• Overview of Higgs Searches
• Search Strategies:
– Standard Model Higgs
• Low and High Mass regions
– SUSY Higgs
– ttbarH production
– Diffractive Production
• Future Prospects
• Conclusions
Constraints on the Higgs Mass
• Direct Searches at LEP
• Fits to Precision Electroweak Data
• Fit for the Higgs Mass (LEP EWWG 2001)
SM Higgs Production at Tevatron
Gluon fusion
Associated Production
typical production cross-sections
s[pb] (mH=100 GeV)
gg H
WH
ZH
1.0
0.3
0.18
WZ
Wbb
3.2
11
tt
tb+tq+tbq
QCD
7.5
3.4
O(106)
WZ/ZH production is cleanest
SM Higgs Decays and BRs
•Divide into two regions
•Low Mass
–H-.bb domintaes
–gg->H precluded by
QCD background
•High Mass
–Gauge Boson decays
dominate
–H->WW becomes
promising
•Less sensitivity in cross over region
Low Mass Higgs Search

•Higgs couples most strongly to massive particles:
•Focus on associated production (WH/ZH)
– Best Prospects: leptonic W/Z decays
– QCD background large
for hadronic channels
•SM Background processes:
•Sensitivity will depend on
–b-jet tagging
– dijet mass resolution
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1
2 3
SM Higgs: Leptonic Channel (1)
• Typical Selection:
•Main backgrounds:
•Event selection optimized to maximize S/B
Expected Events and Sensitivity
Sensitivity crucially depends
on dijet mass resolutions
Mass Resolutions: cont’d
•Signal significance depends on bb mass resolution
–For RunII aim for 10% mass resolution
–30% better than in the previous Run
WHlnbb
CDF RunI
“Calibration for Higgs Search
Mass Resolutions: cont’d
• Run I Jet ET resolution vs
Fast MC
• Optimize b-jet reconstruction
and corrections
• corrections (partly for b’s):
– b/light-q jet calibration
• Improvement due to increased
+jets statistics
• Significant sample of Z bb
– Correct for n in bln
– Correct for  in jets
• Can get 12% at M=120 GeV
– If only 12% mass resolution
• Required luminosity increases
by 20%
WHlnbb
Mass resolution issues
•Problem is not intrinsic jet resolution
–In 2 jet WH events, Mjj is close to gaussian
•Mass resolution is about 10% (but, costs 30-70% in efficiency)
–With 2 jet requirement relaxed,
•Mass resolution is about 15%
3rd jet must be
judiciously used!
More improvements – b-tagging
•b-jet tagging: Will it be good enough?
–Displaced Vertices
•secondary vtx  2 tracks
•tagged if Lxy/s Lxy >3.0
•3-D vs 2D vertexing possible
•Improved impact parameter resolution
•(Extrapolation from CDF Run I eff.)
–Semileptonic tags
e or  in jet
b
b-tagging
can we improve?
•For bb backgrounds:
•Relative Luminosity goes as
• Eff increase from 60%  65%
would result in the same signal
significance for 20% less
integrated luminosity.
LEP2, S.Jin
PHENO2000
Multivariate Analysis techniques
•Further Improvements from use of Neural
Networks, Grid Search, likelihood methods.
– Significant gains, compare S/B
with and without neural nets
SM Higgs: Leptonic Channel (2)
• Main backgrounds:
•Event selection optimized to maximize S/B
•Typical Selection:
•Some distributions:
•Use Neural Networks to optimize analysis:
– use different networks
• one for signal
• 4 different ones for bkg
SM Higgs: Leptonic Channel (3)
•Small rate but good S/B
•Main backgrounds:
•Typical Selection:
•Neural Network Analysis:
•signal
•Backgrounds
(4 different networks)
•Kinematic fit may enhance sensitivity
•Add Taus?
Low Mass Higgs Search
•It’s going to be challenging…
A 120 GeV Higgs signal
Total Background
Conclusion
Tevatron Run II
precision studies of top quark properties
LHC… `top factory’
open possibilities of new measurements
e.g. Yukawa coupling, rare decays, CP
violation etc.
Thanks to
CDF and DØ collaborations
WH: Leptonic Channels
Distributions
bb mass reconstruction
the extracted signal significance depends on input dijet mass resolution
optimized b-jet reconstruction+corrections
WHlnbb
E. Barberis
improvement from use of tracking and preshower
in jet reconstruction? (also, different algorithms?)
corrections (partly specific to b’s):
- corrections for n into jets (bln)
and...
- corrections for  into jets
-effect of extra interactions
- b/light-q jet calibration
on jet reconstruction
- b/light-q parton corrections
b-tagging
•displaced vertices:
RunI SVX algorithms on RunII
detector (3D Si, large h)
secondary
vtx
fakes:
~55-60%
Lxy
primary
vtx
do
•secondary vtx  2 tracks
•tagged if Lxy/s Lxy >3.0
M.Roco
+ soft lepton tagging (~10%)
e or  in jet
b
DØ used only ‘s in top analyses
M.Roco
Low Mass Higgs Searches
•Channels: