Title: Jet Physics in ALICE
1Jet Physics in ALICE
- Mercedes López Noriega - CERN
- for the ALICE Collaboration
Hot Quarks 2006 Villasimius, Sardinia - Italy
2Physics motivation
- High energy partons, resulting from an initial
hard scattering, will create a high energy
collimated spray of particles ? jets - Partons traveling through a dense color medium
are expected to lose energy via medium induced
gluon radiation, jet quenching, and the
magnitude of the energy loss depends on the gluon
density of the medium - Total jet energy is conserved, but quenching
changes the jet structure and fragmentation
function
Measurement of the parton fragmentation products
reveals information about the QCD medium
3Outline
- Partonic energy loss at RHIC
- Jet Rates at the LHC
- Full reconstruction of jets
- Reconstructing jets in ALICE
- Jet observables
- Conclusion
4Results from RHIC
Evidence for partonic energy loss in heavy ion
collisions
High-pT suppression in central AuAu collisions
High-pT hadrons of recoiling jet suppressed in
AuAu but not in dAu
5Full jet reconstruction
Leading Particle
- Leading particle becomes fragile as a probe
- Surface emission
- Small sensitivity of RAA to medium properties.
- For increasing in medium path length L, the
momentum of the leading particle is less and less
correlated with the original parton 4-momentum.
Reconstructed Jet
- Ideally, the analysis of reconstructed jets will
allow us to measure the original parton
4-momentum and the jet structure. - ? Study the properties of the medium through
modifications of the jet structure - Decrease of particles with high z, increase of
particles with low z - Broadening of the momentum distribution
perpendicular to jet axis
6Jet rates at the LHC
- Huge jet statistics from ET 10 GeV
to ET200 GeV - Jets with ET gt 50 GeV will allow full
reconstruction of hadronic jets, even in the
underlying heavy-ion environment. - Multijet production per event extents to 20 GeV
7ALICEA Large Ion Collider Experiment
Central PbPb Collisions at vs 5.5 TeV dNch/dy
2000-8000 dET/dh 1.5-6 TeV
- Central barrel hlt 0.9
- High-pT capabilities
- High pT charged hadrons identification
- Momentum resolution better than 10 up to 100
GeV/c - Photons
- Proposed electromagnetic calorimeter
- p/3 lt F lt p
- h lt 0.7
- Energy resolution 15
8Jet reconstruction in ALICE
- In pp-collisions
- jets excess of transverse energy within a
typical cone of R 1. - In heavy-ion collisions
- jets reconstructed using smaller cone sizes
- subtract energy from underlying event
- Main limitations
- Background energy. Reduced by
- reducing the cone size (R 0.3-0.4)
- transverse momentum cut (pT 1-2 GeV/c)
- Background energy fluctuations
- event-by-event fluctuations
- Poissonian fluctuations of uncorrelated
particles - fluctuations of correlated particles
- Collimation 80 energy around jet axis in R lt
0.3 - Background energy in cone of size R is R2 and
background fluctuations R.
9Intrinsic performance
ET 100 GeV, R 0.4
- Limited cone size leads to a low energy tail
- Charged reconstruction (TPC) dominated by
charged to neutral fluctuations
- Background energy contained in a subcone of
radius R reduced by - reducing the cone size
- cutting on pT
10Reconstructed ET-spectrum
107 central events R 0.4 Charged jets
- Study properties of the medium through the
modifications on the transverse jet structure - Jet shape (dE/dr) and jet particle momentum
perpendicular to jet axis (jt) vs. reconstructed
energy - Study hard processes with low pT observables by
measuring the fragmentation function to low pT.
Energy loss and radiated energy - Decrease of hadrons in the high-z part and
increase of hadrons in the low-z region of
fragmentation function (z pT/ETjet)
11Jet shape and jT
Salgado, Wiedemann, Phys.Rev.Lett.93, 042301
(2004)
Fraction of energy in a subcone of radius
R. Lowering p parallel to the axis increasing p
perpendicular to axis ? increase of the jet size
- Fraction of energy in a subcone of radius R.
Differences are difficult to measure but ?
increase on mean jT
12Hump-backed Plateau
Representing the fragmentation function
Hump-backed Plateau. Charged jets.
Particles from medium induced gluon radiation in
? 4-6 For ET 100 GeV, S/B 10-2
Leading Particles S/B gt 0.1
13RHIC like analysis
Trigger 4 lt pT lt 8 GeV/c Assoc. pT lt 4 GeV/
in steps of 0.5 GeV/c
0 lt pTassoc lt 0.5
0.5 lt pTassoc lt 1.0
1.0 lt pTassoc lt 1.5
1.5 lt pTassoc lt 2.0
2.0 lt pTassoc lt 2.5
2.5 lt pTassoc lt 3.0
3.0 lt pTassoc lt 3.5
3.5 lt pTassoc lt 4.0
pp events at vsNN 14 TeV. Fully
reconstructed events.
14Conclusion
- Copious production of jets in PbPb collisions at
the LHC - ALICE will be able to identify jets
- in reduced cones R 0.3-0.5 to reduce
contributions from the underlying event - the proposed EMCal will improved jet
reconstruction - ALICE will study the properties of the medium
through the jet structure observables (radiated
energy is observed in low-pT particles) - jet shape increase on the jet size
- momentum perpendicular to the jet axis, jT
increase of mean value, broadening of the
distribution - fragmentation function increase on the number of
particles with low z and decrease on the number
of particles with high z - ALICE will also
- study the dependence of the energy loss in
particle species - study gamma-jet correlations
15Backup Slides
16Out-of-cone fluctuations
ET 100 GeV
17Production rate weighted resolution function
- Intrinsic resolution limited to DE/E (15-20)
- Production rate changes factor of 3 within DE
- Production rate weighted resolution function has
to be studied.
Input spectrum for different cone energy of
charged jets.
18Jet-structure observables
Jet particle momentum perpendicular to jet axis
(jt)
Salgado, Wiedemann, hep-ph/0310079
19Photon-tagged jets
- g-jet correlation
- Eg Ejet
- Opposite direction
- Direct photons are not perturbed by the medium
- Parton in-medium-modification through the
fragmentation function
20Prompt g-hadron correlations
- Azimuthal Correlation in pp collisions at LHC
energies (PYTHIA). - Trigger particle Highest pT g.
- Associated particle Charged particles with pT gt
1 GeV/c.
Prompt g - hadron
p0 - hadron
Useful to estimate the fraction of decay photons
present in the experiment
21RHIC like analysis?
Trigger 5 lt pT lt 8 GeV/c Assoc. pT lt 5 GeV/
in steps of 0.5 GeV/c
Pythia events.