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Outline

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Apply jet energy corrections (same as in Run I) Largest uncertainty ... Data samples w/ higher statistics than Run I. Dominant systematic: jet E-scale ... – PowerPoint PPT presentation

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Title: Outline


1
Jet studies at CDF in Run II
La ThuileFri. Mar. 14, 2003
Rob Snihur University College London for the CDF
collaboration
  • Outline
  • Motivation
  • Inclusive jet cross section
  • Dijet mass
  • Jet shapes
  • Summary

2
Motivation
  • Tevatron jet factory
  • Probe highest energy scales
  • Higher vs ? higher s (factor 3 for ET gt 500 GeV)
  • Already more jets than in Run I
  • Test fixed-order QCD
  • look for deviations ? new physics
  • Constrain PDFs
  • Analyses
  • Inclusive jet cross section (counting jets)
  • Dijet Mass (bump hunting)
  • Jet Shapes Energy Flow

3
Tevatron CDF
Upgraded Tevatron at Fermilabvs 1.8 TeV ?
1.96 TeV Higher s(jet)
NLO QCD
s(jet) ratio Run II / Run I
  • Collider Detector at Fermilab (CDF)
  • New plug calorimeter (1.1 lt h lt 3.6)
  • New tracking system
  • Upgraded trigger

jet ET (GeV)
4
Highest Energy Jets in Run II
Jet 2 ET 546 GeV (raw) hdet -0.30
Jet 1 ET 583 GeV (raw) hdet 0.31
  • Run 152507 Event 1222318
  • Dijet Mass 1364 GeV (corr)

CDF Run II Preliminary
5
Inclusive Jet Cross Section
  • Repeat Run I analyses
  • Use CDF cone jet algorithm with R 0.7 (JetClu)
  • Event selection cuts
  • zvertex lt 60 cm
  • ? ET lt 1500 GeV
  • Require fully efficient trigger
  • Apply jet energy corrections (same as in Run I)

6
Systematic Uncertainties
Luminosity uncertainty 6
Largest uncertainty
7
Corrected Log
  • 8 orders of magnitude!
  • Highest ET jets ever!

CTEQ 6.1 hep-ph/0303013
8
Corrected Linear
CDF Run II Preliminary
JetClu cone R 0.7, vs 1.96 TeV

s ratio Data / CTEQ6.1
CDF data

5 Energy scale uncertainty
CTEQ 6.1 uncertainty
Inclusive jet ET (GeV)
Good agreement (within uncertainties)
9
Run II I
  • Higher s in Run II due to higher vs
  • Many uncertainties cancel in the ratio

10
Dijet Mass
  • Higher s in Run II due to higher vs
  • 3 more bins at high dijet mass!

11
Run II I
Consistent with inclusive jet cross section
12
Limits
13
Jet Shapes
narrow
?(r)
fat
r
Differential jet shape definition
14
Data HERWIG
CDF Run II Preliminary
  • Narrower jets at high ET low ?
  • HERWIG agrees well with data

15
Calorimeter vs. tracking
CDF Run II Preliminary
  • Use COT tracks with pT gt 0.5 GeV
  • Agrees with calorimeter-based shape
  • Agrees with PYTHIA

16
Energy flows
  • Look outside the jet
  • Probe the underlying event

17
Energy flows
CDF Run II Preliminary
Increasing ??jet
Increasing ?jet
18
Summary
  • CDF has preliminary measurements in Run II
  • Inclusive jet cross section
  • Dijet mass
  • Jet shapes energy flow
  • Higher vs ? more jets at high ET
  • Data samples w/ higher statistics than Run I
  • Dominant systematic jet E-scale
  • General agreement w/ fixed-order QCD calculations
    Monte Carlos

19
Outlook
  • Reduced systematics
  • More data
  • Forward jets
  • Different jet algorithms
  • Other jet analyses
  • Dijet angular distribution
  • s(b-jet)
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