Title: The KT Algorithm at D
1The KT Algorithm at DØ
- Veronica Sorin
- Universidad de Buenos Aires
2Outline
- Jet Algorithms
- KT Jet Algorithm at DØ
- Calibration of KT jets
- Physics Analyses
- Summary
3Jet Algorithms
- Parton jet q and g (before hadronization)
- Particle jet final state particles (after
hadronization) - Calorimeter jet measured object (after
calorimeter shower)
Fixed Cone (RunI) KT (Ellis-Soper)
Iterative
Fixed cone of radius R
Overlapping cones split/merge
parameter Sensitivity to soft radiation
Recombination Distance parameter D
Infrared and collinear safe
4KT Algorithm at DØ (RunI)
Input List of preclusters
Is less than ?
Yes
Merge ij
No
Move i to list of jets
Anyleft?
Yes
No
5Jet Momentum Scale Correction
Calorimeter jet
Particle jet
- Offset (O) Ur noise, pileup, multiple
interactions, underlying event (ue) - Response (Rjet) Pmeas / Ptrue
- (using transverse momentum balance in g-jet
events)
No Showering correction (showering losses outside
cone)
6Luminosity dependent
. .
.
N(GeV)
UE(GeV)
3
1
2
1
D1.0
D1.0
30 lt PTlt 50 GeV
30 lt PT lt 50 GeV
h
h
2
1
1
2
Herwig detector simulation Overlayed to random
crossing
Herwig detector simulation Overlayed to
crossing with inelastic interaction
7Rjet Correction
Monte Carlo Closure
Rjet a b ln(Pjet) c ln2(Pjet)
Rjet
0.9
D1 (KT jets)
0.75
0
Pjet (GeV)
0
300
8Jet Structure
Subject Multiplicity (M) for quark and
gluons Test of QCD, discriminating variable to
tag quark jets in the final state
Cone jet
D0 Preliminary
KT jet
Re-run KT algorithm on all 4-vectors merged
into a jet
9 Event Shapes
Thrust
Test QCD, Extraction of as , Non-perturbative
corrections
Jet Production (Inclusive Jet Cross Section ,
Sebastian Grinstein )
10Summary
- KT Jet Algorithm has successfully been
implemented and calibrated at DØ - Analyses in progress
- Improvements for RunII
Jet Algorithms http//www.physics.niu.edu/blazey/
jet_alg/jet_alg.html