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Top Mass in the all hadronic channel

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... G. Lungu, S. Sukhanov Florida University. Mass Workshop June 23 ... Work in progress to evaluate a priori how well we can do in different luminosity ... – PowerPoint PPT presentation

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Title: Top Mass in the all hadronic channel


1
Top Mass in the all hadronic channel
  • P. Azzi, T. Dorigo - Padova University INFN
  • Castro, A. Gresele Bologna University INFN
  • I. Lazzizzera, S. Amerio Trento University
    INFN
  • J. Konigsberg, G. Lungu, S. Sukhanov Florida
    University
  • Run I analysis strategy
  • Mass Reconstruction in RunI
  • Status with RunII MC and data
  • Plans

2
Run I analysis strategy
  • The all hadronic channel
  • BR is large (46) ?
  • Events fully reconstructable ?
  • Large QCD background S/B is very small ?
  • RunI Analysis had to cope with low statistics and
    a low double b-tagging efficiency
  • Specific trigger was developed S/B _at_trigger
    1/500
  • Two paths for improving S/B
  • A)Tight Kinematic gt1 btag S/B 1/4
  • used for mass measurement
  • B) Loose Kinematic gt2 btag S/B 1/4

3
Run I Analysis Strategy (contd)
Multijet Trigger Data Sample
Large Jet Multiplicity Large Total Transverse
Energy One B-tag jet present
  • Kinematic Cuts
  • Centrality
  • Aplanarity

Two B-tagged jets
Cross Section s7.63.5-2.7 pb
Mass Reconstruction M(t)186105.7 GeV/c2
4
Run I Event Selection for Mass Reconstruction
  • Jet counting definition
  • Et(raw)gt15 GeV etalt2
  • Main background QCD 2?2 processes with extra
    jets due to gluon radiation
  • Kinematic very different from tt
  • Use data before tag for the background shape
  • Signal contamination negligible
  • Cuts (corrected jet energies)
  • 6?N(jet)? 8
  • ?Et? 200 GeV
  • ?Et/?s?0.75 (centrality)
  • Aplanarity0.0025 x ?3Et ?0.54

ltM(t)gt
175
SET
The ?Et cut has been lowered wrt to the value
optimized for the cross section selection b/c of
its bias on the background shape
5
Mass Measurement in RunI
  • Fully reconstructable final state
  • Fit the six jets events to tt
    hypotesis (3
    constraints)
  • M(jjb)1 M(jjj)2
  • M(jj)1M(W)
  • M(jj)2M(W)
  • Combinations
  • No tag 90
  • 1 Tag 30
  • 2 Tag 6
  • Caveat even in events with two tags we required
    only one of the b to be associated to the parton.
    In 30 of the cases the second tag is a charm
    from W decay.
  • In Run I we saw no significant improvement in
    top mass resolution from 1 to 2 tags

One b
Two b
6
Mass Measurement in Run I (contd)
Double tagged events (consistency check)
M(t)186105.7 GeV/c2
7
Run I Systematics
Final weights in the combined mass result 0.65
(ljets), 0.19(dilepton), 0.15 (hadronic)
8
The RunII trigger and datasets
  • Dedicated trigger TOP_MULTI_JET (after Run
    143938)
  • Requires N(jet)gt4 with Etgt15 and ?Etgt125 GeV
  • Before Run 143938 L2 was only ?Etgt130 GeV cut
  • Total luminosity available now is ?Lint107 pb-1
    (with good run list and SVX requirement)
  • Available datasets (Andrea C.)
  • Events before Jan shutdown processed with
    4.9.1hpt1
  • Full statistics up to May27th processed with
    4.11.1
  • Signal MC use official tt MC of the Top Group
    (inclusive)

9
Work in progress and plans
  • Top Hadronic Group meets informally every two
    weeks
  • Basic philosophy for RunII analysis
  • Full characterization of the multi-jet datasets
    (Njetgt4) in terms of kinematical properties and
    heavy flavor content
  • Currently we are validating data after the
    shutdown
  • Use of new tools (ME MC such as Alpgen) to have
    an extra handle on the background determination
  • In Run I no MC was available to properly describe
    high multiplicity events with heavy flavor
  • Optimize analysis selection for a S/B1/1 (or
    better) in the signal region
  • Work in progress to evaluate a priori how well we
    can do in different luminosity scenarios

10
First look using Run II MC
  • Machinery for mass reconstruction is already in
    place.
  • Work in progress to add top specific corrections
  • Run II Herwig MC
  • Jet corrected to Level7
  • Compare the resolution for tt in the case of 0, 1
    and 2 tags
  • In RunI width was 24 GeV(22 GeV) with 0tag (1
    tag) with full AA corrections.

11
Comparison Run I vs Run II background shape
Entries1153
RUN II multi-jet data 0 tag after kinematical
selection Top specific corrections missing!
RUN I multi-jet data 0 tag after kinematical
selection Full Run I jet corrections
12
Run II signal and background shape
  • After a Run I style kinematical selection
  • 0 tag (veto) S/B 1/100 , negligible top
    contribution
  • gt 1 tag S/B1/6
  • gt2 tags S/B1/1

13
Future Plans
  • Work in progress to reoptimize analysis to take
    full advantage of the CDF upgraded detector and
    increased statistics
  • Need to fully characterize (again)
  • Correlations of kinematical and b-tagging
    requirement
  • Issues on mass reconstruction from the 2 tags
    requirement
  • Background shape?
  • improvements in resolution?
  • Other ideas bottom/charm difference? Interplay
    of different b-taggers?
  • Plan is to have a preliminary results for this
    Winter
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