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ALICE at LHC

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Energy density (5 GeV/fm3) well beyond critical value ... quarks (3 flavors) and gluons with restored Chiral ... The hard parton is thermalised in the heat bath ... – PowerPoint PPT presentation

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Title: ALICE at LHC


1
ALICE at LHC
  • New states of matter ? (QGP, wQGP, sQGP, bsQGP,
    CGC,)
  • New probes

LHC not relevant for the search of the critical
point Marek Gazdzicki
2
SPS New State of Matter created at CERN (10
Feb. 2000)
PbPb vsNN 17.3 GeV NA 49
  • 7 dedicated experiments (NAxx, WAyy)
  • Compelling evidence for the existence of a new
    state of matter (e 3.2 GeV/fm3gtec, strangeness
    enhancement, J/? suppression, direct thermal
    photon radiation,)
  • Interpretation in terms of QGP formation not
    unique

3
RHIC The discovery of the QGP at RHIC (M.
Gyulassy QM 2004)
  • 4 multipurpose experiments (BRAHMS, PHENIX,
    PHOBOS, STAR)
  • Empirical lines of evidence
  • Energy density (5 GeV/fm3) well beyond critical
    value
  • Large elliptic flow early collective behavior at
    partonic level
  • Jet quenching, mono jets absorption of partons
    in a color dense opaque medium
  • dA control experiment
  • Interpreted in terms of a strongly coupled QGP
    and a new QCD state (?) Color Glass Condensate

AuAu vsNN 200 GeV STAR
4
LHC The closest approximation of the Big Bang
It is dangerous to make predictions, especially
about the future."
  • One heavy ion experiment, ALICE
  • In 04/2007, LHC will deliver first pp at 14 TeV
    collisions,
  • and soon after PbPb collisions at vsNN 5.5 TeV.

5
What will be new at LHC








few 105 bigger






10 longer
30-40 longer





15-60 denser




3.0-4.2 hotter



0.1 faster


1000-4000 ?

5500 X 28
SPS RHIC LHC
vsNN (GeV) 17 200
dNch/dy 500 850
t0QGP (fm/c) 1 0.2
T/Tc 1.1 1.9
e (GeV/fm3) 3 5
tQGP (fm/c) 2 2-4
tf (fm/c) 10 20-30
Vf(fm3) few 103 few 104
The biggest step in energy in the history of
heavy-ion collisions
6
Formation of the real vacuum of QCD
  • Weakly interacting gas of mass less quarks (3
    flavors) and gluons with restored Chiral
    symmetry

Not yet a StefanBoltzmann gas
RHIC
as(T)4p/(18log(5T/Tc))
LHC
SPS
mu md ms mu md mu md ms ? mu,d HQ
suppressed exp(-mc,b,t/T)
7
A new kinematical regime
108 106 104 102 100
  • xltlt1
  • Determines the properties of the medium
    (QS0.2A1/6vsd 2.7 GeV)
  • The QGP at LHC might evolve from a Color Glass
    Condensate in the initial state of the collision

Q2 (GeV2)
LHC The color glass machine L. McLerran 
ALICE PPR CERN/LHCC 2003-049²
8
A new kinematical regime
  • Q gtgt 1
  • Determines the probe of the medium
  • Q gtgt LQCD, T (Dt, Dr 1/Q) pt gt 2 GeV/c

9
Hard probes
  • Particle production dominated by hard processes
  • Heavy quarks and weakly interacting probes become
    accessible
  • Happen at t0 ? initial stage of the collision
  • Have a large virtuality ? short formation time
  • Probe matter at very early times ? QGP
  • Can be calculated by pQCD ? predictions

LHC shard/stotal 98 (50 at RHIC)
10
Dynamics of hadronisation in vacuum
hadronic final state
ET
Lhadr ET/Q2hadr
  • The medium modifies the vacuum dynamics
  • Modifications are imprinted in the hadronic final
    state

11
Dynamics of hadronisation in medium
hadronic final state
ET
Lhadr ET/Q2hadr
  • The radiated energy (DE) depends on the
    properties of the
  • medium (the transport coefficient q)
  • The competition between thermalisation (DEE) and
  • hadronisation depends on the hard parton
    transverse energy.


12
Dynamics of hadronisation in medium
ET
  • Lthermlt Lhadr lt Lmedium
  • The hard parton is thermalised in the heat bath
  • Bulk properties of the medium from low pht ( 2
    GeV/c) hadrons, leptons, photons

13
Bulk properties of the LHC medium
  • Monotonic extrapolation from RHIC but changes in
  • Expansion dynamics and (elliptic flow, transverse
    volume, event by event fluctuations, )
  • Freeze out (temperature, charm, )
  • Thermal photons (real virtual)

14
Dynamics of hadronisation in medium
hadronic final state
ET
Lhadr ET/Q2hadr
  • Ltherm Lhadr Lmedium
  • The medium is a tool to modify the hadronisation
    process
  • Dynamics of hadronisation (pht 2-7 GeV/c)

15
Medium modified fragmentation
p/p
PtGeV/c
  • Fragmentation, recombination ?

16
Dynamics of hadronisation in medium
xET
hadronic final state
ET
  • Lthermgt Lhadr gt Lmedium
  • The parton looses additional energy (qL2)
  • The multiplicity, transverse momentum of the
    shower broadens (qL)
  • Leading hadron



17
Leading hadron (qL2)

Eskola, Honkanen, Salgado, Wiedemann
Nucl Phys A, hep-ph/0406319
  • Probe the reduced energy of the parton with the
    reduced energy of the leading hadron.
  • But surface emission limits the sensitivity to
    the medium properties

18
Mass and color charge dependence
19
Jet heating (qL)
  • At LHC jets can be reconstructed in the HI
    environment
  • The measurement of the jet structure provides a
    better sensitivity to the medium properties

20
Jet heating
. kt
  • Sensitivity of jet energy distribution weak
  • Broadening of kt
  • Modified longitudinal fragmentation function
    g(Z)-jet tagging

21
g-jet tagging
PbPb 40GeV ? g-jet R0.3 ptgt 2 GeV/c
Ejet/Eg
22
12 experiments at the LHC
ALICE
ATLAS
CMS
23
ALICE Physics Program
  • Deconfinement
  • charmonium and bottomonium spectroscopy
  • Energy loss of partons in quark gluon plasma
  • jet quenching high pt spectra
  • open charm and open beauty
  • Chiral symmetry restoration
  • neutral to charged ratios
  • resonance decays
  • Fluctuation phenomena - critical behavior
  • event-by-event (vN) particle composition and
    spectra
  • pp collisions in a new energy domain

24
Heavy ion experiment at LHC
  • ALICE will meet the challenge to measure flavor
    content and phase-space distribution
    event-by-event
  • Most (2p 1.8 units h) of the hadrons (dE/dx
    ToF), leptons (dE/dx, transition radiation,
    magnetic analysis) and photons (high resolution
    EM calorimetry)
  • Track and identify from very low (lt 100 MeV/c
    soft processes) up to very high pt (gt100 GeV/c
    hard processes)
  • Identify short lived particles (hyperons, D/B
    meson) through secondary vertex detection
  • Identify jets

25
ALICE PID
Alice uses all known techniques!
p/K
TPC ITS (dE/dx)
K/p
e /p
p/K
e /p
TOF
K/p
p/K
HMPID (RICH)
K/p
0 1 2
3 4
5 p (GeV/c)
TRD e /p
PHOS g /p0
EMCAL
1 10
100 p (GeV/c)
26
Jet Phase Space
Jet physics will dominate the LHC heavy-ion
program, ALICE will be the main contender of the
race for jet quenching
Qs
TLQCD
Mini-jets 100/event
100K/year
1/event
Bulk properties
Hard processes Modified by the medium
ALICE Tracking PID
Jets from Correlations and Leading Particles
Reconstructed Jets
27
ALICE
28
The ALICE program in 2007 on wards
sPbPb 8barn LPbPb 1027cm-2s-1 t004/2007
  • The first 15 minutes Lint1mb-1
  • Event multiplicity, low pt hadronic spectra,
    particle ratios
  • The first month Lint0.1-1nb-1
  • Rare high pt processes jets, D,B, quarkonia,
    photons, electrons
  • The following years
  • pA, A scan, E scan

29
(No Transcript)
30
ALICE the dedicated HI experiment
Cosmic rays trigger
  • Forward detectors
  • PMD
  • FMD, T0, V0, ZDC
  • Specialized detectors
  • HMPID
  • PHOS
  • Central tracking system
  • ITS
  • TPC
  • TRD
  • TOF
  • MUON Spectrometer
  • absorbers
  • tracking stations
  • trigger chambers
  • dipole

31
Proposed ALICE EMCAL
  • EM Sampling Calorimeter (STAR Design)
  • Pb-scintillator linear response
  • -0.7 lt h lt 0.7
  • p/3 lt F lt p
  • Energy resolution 15/vE
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