Title: The heavy ion collider experiment @ LHC A L I C E
1The heavy ion collider experiment _at_ LHC A L I C E
- Ginés MARTINEZ
- for the ALICE Collaboration
Photon Group _at_ SUBATECH(IN2P3/CNRS ENM - UN)
Nantes, France
2Outlook
- Why a Heavy Ion Experiment _at_ LHC?
- Goals
- Building ALICE
3The study of the Quark Gluon Plasma
Krasch QM2001
Lattice QCD calculations nf2 Tc 1738SysErr
MeV nf3 Tc 1538SysErr MeV ec 700 300 MeV
- QCD-thermodynamics
- Properties of the QGP and of the phase
transition - Chiral transition
- Deconfinement
4Towards QCD thermodynamics
- The TOOLS
- Heavy Ion Collisions SPS gt RHIC gt LHC
- The relation with QCD at finite temperature
- The pp pA baseline
- Equilibration
- Probes of QGP formation?
- QGP Initial conditions?
Collision dynamics
5collision dynamics
pp and pA baseline !
Sensitivity to late stages in HI collisions!
Final state probes
Penetrating probes
The QGP phase
6Why HI program _at_ LHC ?
Central collisions SPS RHIC LHC
s1/2(GeV) 17 200 5500
dNch/dy 500 700-1500 3-8 x103
e (GeV/fm3) 2.5 3.5-7.5 15-40
Vf(fm3) 103 7x103 2x104
tQGP (fm/c) lt1 1.5-4.0 4-10
t0 (fm/c) 1 0.5 lt0.2
_at_ LHC Hotter bigger - longer
J. Schukraft QM2001
7The gluon-gluon physics
- Gluon distribution in nuclei grows for small
values of x 2pT /s1/2 and high gluon densities
are reached . - For high densities (rT gtgt L2QCD ) in large nuclei
small x, the gluon distribution can be
computed in the weak coupling method. - The classical color field.
- A large number of gluons are freed in the early
stage of the collision gt Equilibration
PRD10(74)1649, PRC49(94)2233, PRD49(94)3352,
PRD53(96)458, PRC56(97)2219
8Advantages of PbPb collisions _at_ LHC
- Better connection with QCD theory (via the
asymptotically free field theory) A E - Initial gluon multiplicity (R.Venugopalan QM01,
PRL86(01)1717) - Initial equilibration conditions (D. Son
QM01,hep-ph/0009237) - Longer lifetime of the plasma
- Ideal plasma e/ec 5 higher T
- Zero baryon density (already p/p 0.6 _at_ RHIC)
- New probes Jets, Open charm beauty,
bottonium
9Final state probes
- Forward energy
- dN/dy
- hadron pT distribution
- Particle ratios
- Strange particles
- Multiplicity
- Energy Density
- HBT and dynamical evolution
- Freeze-out temperature
- Fluctuations
- Collective motion
- 12200 ps
- 1700 Ks
- 700 hs
- 570 p, n, p, n s
- .
-1lthlt1
PbPb _at_ 5.5A TeV
10Penetrating probes
- Real and virtual photons
- Quarkonia J/Y Y
- Open Charm Beauty
- Light vector mesons
- Jets
- Initial stage
- Thermal radiation Tini
- Colour screening of heavy quarks
- Jet-matter interaction
- Chiral transition
11Jet Matter interaction
1-3 GeV/fm
Large production of jets _at_ LHC energies 1
jet/GeV/s in the ALICE acceptance at ET 50 GeV
Dt0
B
A
Looking for Jet matter interaction
- High pT particle distributions
- Identification of jets
- Tagging with photons
- High pT particles
- Jets
g
Interference with vacuum and LPM, Jet
enhancement Ejet dependence of DE pTgt 10 20 GeV
Urs. Wiedemann QM2001 et NPB588(00)203
12Building ALICE
- Event Characterisation
- dNch/dy
- pT distribution
- Particle ratios
- Strange baryons
- Fluctuations
- Light vector mesons
- Quarkonium
- Open charm beauty
- Photon Dilepton
- Jet quenching
13dNch/dh Dh1 8000
Tracking efficiency 90 2 tracks eff. 80 Dpgt15
MeV/c
- Time Projection Chamber Main tracking
detector of ALICE central barrel - Inner radius Track separation
- Rin 0.8 m
- Outer radius dE/dx p resolution Rout
2.5 m - Large acceptance Dh lt0.9
- 200Hz rate capability
- MWPC read-out 32 m2, 40 Oc
- 5 105 pads x 500 time bins
- 60 Mbyte/evt gt DC, RoI, L3
5 m
TPC
NeCO2(10)
- PID below 600 MeV/c
- Low Dp tracks
Magnetic field of the L3 magnet 0.4T 5 _at_ 5
GeV/c
14The ALICE PID
Time of Flight High Momentum Particle
Identification Transition Radiation Detector
- 0.5 lt p lt 5 GeV/c
- e, p, K, p
ALICE solution
ToF prototype
Multigap Resistive Plate Chamber
- pT distributions
- Particles ratios Tfreeze-out
- Fluctuations
- Strangeness production
- Light vector mesons
- Open charm
- Jet physics
ToF
- Large acceptance
- MRPC
- s 150 ps
- p,K,p
- 0.5ltplt2.5 GeV/c
10cm
15High momentum particles
- High Momentum PID
- Hard processes
- 1 GeV/c lt p lt 5 GeV/c
- Rich-imaging technique
- Small acceptance
7x
HMPID
16Electron Identificator of ALICE
- Electron detector
- 10-3 pion rejection
- Large acceptance
- Transition Radiation Detector
- J/Y in Zero baryon density
- Open charm normalization
- J/Y source from Open Beauty
- D annihilation?
- G production
- Light vector resonances f, w
e channel
TRD
PbPb central collisions
6x
g 103 EX 3-30 KeV
17Primary and secondary Vertex Position
p
L
- Secondary vertex from hyperon decays
- Open charm beauty physics
- Tracking of low pT particles
- Improving momentum resolution
- Strangelets
W-
I T S
p-
K-
ITS
- Large acceptance
- 15000 tracks
- s100mm in rf
- 6 Silicon layers
- 2 Silicon Pixel layers
- 2 Silicon Drift layers
- 2 Silicon Strip layers
D gtKp 107 evt
18Photon detection
10
- Thermal radiation
- High pt physics
- Tagged jets
- 1200 g pTgt40 GeV/c
5x
Thermal/Decay
1
PHOS
PHOS Module
5
0.1
hep-ph/9906325
pT(GeV/c)
1
2
3
4
- EM calorimeter
- PbWO4 spectrometer p0,h
- Small acceptance 0.07 DhDf/2p
- 1lt pT lt 5 GeV/c
- 5lt pT lt100 GeV/c
19Di muon channel
- Quarkonium physics
- J/Y and Y families
- 100 MeV
- 2.4 lt h lt 4.0
DiMuon
- em coin.
- Intermediate
- rapidity
- DD, BB
- production
20ALICE The result of QGP physics requirements
at LHC
PMD FMD CASTOR ZDC Trigger DAQ Offline
21Running conditions
- PbPb _at_ 5.5A TeV
- 106s per year
- 8000 Hz (L1027 cm-2s-1)
- Data rate full ALICE 50 Hz (TPC challenge)
- pp pA running
- Lighter ions _at_ higher luminosity.
- Beginning 2007
22conclusions
- HI in LHC a rigorous step towards the QGP
physics - Perturbative weak coupling methods
- Direct partonic probes Jets.
- The LHC HI dedicated experiment ALICE
- Penetrating and final state probes
- 884 members 28 countries 77 institutes
- Rendez-vous _at_ CERN March-April 2007
23A new research domain
Quark Matter 2002 in Nantes