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Event by Event Fluctuations in the NA49 Experiment

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Title: Event by Event Fluctuations in the NA49 Experiment


1
Event -by- Event Fluctuations in the NA49
Experiment
  • P. Christakoglou, A. Petridis, M. Vassiliou
  • Athens University
  • For the NA49 Collaboration
  • SPHIC06, Catania
    27-29 Sept. 2006

2
Outline
  • Introduction
  • Energy - Centrality dependence of e-by-e
    fluctuations
  • particle ratio
  • average transverse momentum
  • multiplicity
  • net electric charge
  • System size, rapidity and energy dependence
  • electric charge correlations
  • Conclusions

3
Introduction
  • Event-by-Event measurements offer the
    possibility for studying the QGP phase transition
    and the nature of the QGP matter.
  • PbPb collisions at top SPS energy
  • Initial energy density exceeds the critical value
    predicted by lattice QCD
  • Strong collective behavior
  • Proposed signatures for deconfinement observed
  • Signatures not specific for deconfinement
  • NA49 energy scan 20, 30, 40, 80, 158
    GeV/nucleon
  • To search for structure in the energy dependence
    of hadron production characteristics indicating
    the onset of deconfinement
  • To search for fluctuations which might occur if
    distinct phases coexisted in the early stage of
    the reactions or if hadrons froze out close to
    the critical point.

4
The NA49 Detector
Target 20cm liquid H2 or Pb foil VCAL detects
projectile spectators ?p/p2 7 (0.3) 10-4
(GeV/c)-1 (VTPC-1, VTPCMTPC)
dE/dx resolution 3 6 TOF resolution 60 ps
5
PbPb collision at 158A GeV
6
Particle Ratio Strangeness Fluctuations
  • Since the number of d.o.f in the QGP is lower
    than in a hadron gas ,non-Statistical
    fluctuations of the ?/p ratio could signal
    fluctuations in the fraction of deconfined matter
    at the early stage of the collision.
  • NA49 performed measurements on particle
    ratios in single PbPb collisions at all
    available beam energies.

7
Acceptance
40 GeV
160 GeV
20 GeV
8
The Event-by-Event K/p ratio
Beam Energy
s2dyn s2data s2mixed
9
The K/p ratio Energy dependence
STAR
  • Data Increased fluctuation signal at lower
    beam energies
  • UrQMD ?/p fluctuation signal independent of beam
    energy

10
The Event-by-Event (p p)/p ratio
Beam Energy
The distribution of the E-by-E p/p ratio is
narrower for data than mixed events. Effect of
baryon resonance decay ?
11
The (p p)/p ratio Energy dependence
NA49 preliminary
p/p fluctuation signal in UrQMD closely matches
the energy dependence observed in the data
12
Event-by-event fluctuations of ltpTgt
  • The average transverse momentum in the event is
    related to the Temperature and the Radial flow in
    the fireball, which might fluctuate with the
    initial energy density and the fraction of
    deconfined matter at the early stage of the
    collision.
  • The fluctuation measure

To remove the influence of volume fluctuations,
due to variations of the impact parameter of the
collision
13
Event-by-event fluctuations of ltpTgt
1.1 lt yp lt 2.6
  • distributions of ltpTgt similar
  • for real and mixed events
  • non-statistical (dynamical)
  • fluctuations are small, lt few

14
Centrality and Energy dependence
158A GeV
1.1 lt yp lt 2.6
1.1 lt yp lt 2.6
NA49 preliminary
increase for peripheral collisions, no increase
at lower energy
15
Multiplicity Fluctuations
  • Fluctuations of the charged particle
    multiplicity may be related to fluctuations in
    the initial entropy and the fraction of
    deconfined matter produced in the initial stage
    of the collision
  • Used measure of fluctuations scaled variance
  • 1 for Poissonian distribution

16
Controlling Centrality
AProj
Veto Calorimeter
EVeto(AProj -NPProj)Ekin
NPProj
  • Veto calorimeter -gt projectile spectators, number
    of projectile participants NPProj
  • Target spectators not measured in NA49

17
Multiplicity Fluctuations
1.1 lt y lt 2.6
For non central PbPb coll. the distributions
are wider than the Poissonian one (independent
particle production)
18
Centrality dependence (I)
  • Var(n)/ltngt increases with decreasing centrality
  • Approximate scaling in NPProj/AProj

19
Results II
Centrality dependence (II)
HSD, UrQMD V. Konchakovskyi et al. Phys. Rev.
C 73 (2006) 034902 HIJINGM. Gyulassy, X. N.
Wang Comput. Phys. Commun. 83 (1994) 307
Simulation performed byM. Rybczynski
  • String hadronic models shown (UrQMD, HSD, HIJING)
    do not reproduce data on multiplicity fluctuations

20
Net Charge Fluctuations
  • Net charge fluctuations will be smaller in QGP
    (due to fractional charges of quarks) than
    in gas of hadrons
  • The Fluctuation Measure

21
Net Charge Fluctuations
?Fq Fq - Fq,gcc
QGP signature possibly erased by hadronisation
(Bialas) or the effect of resonance decays
(Zaranek)
22
Charge Correlations -The Balance Function
Bass,Danielewicz,Pratt PRL 85,2689(2000)
  • oppositely charged particles created
  • at the same point in space time
  • particles get separated in rapidity by
  • thermal motion (rescattering) and
  • developing collective flow
  • early produced pairs are separated more
  • in rapidity than late produced pairs
  • separation d? quantified by the
  • balance function

delayed hadronisation
narrowing of balance function predicted as
signature of first order phase
transition
23
System size and centrality dependence - vsNN
17.2 GeV
  • The width takes its maximum value for pp
    interactions.
  • Data show a strong system size and centrality
    dependence.
  • Neither HIJING nor shuffled data show any sign
    of system size or centrality dependence.

C. Alt et al. NA49 collaboration, Phys.Rev.
C71, 034903 (2005).
24
Comparison NA49 STAR
  • NA49 data show a strong centrality dependence of
    the order of (17 3).
  • STAR data show also a strong centrality
    dependence of the order of (14 2).

25
Rapidity dependence - vsNN 17.2 GeV
26
Energy dependence
27
Conclusions
  • NA49 has studied the e-by-e fluctuations
  • The K/p ratio fluctuation signal increases at
    lower SPS energies.
  • The fluctuations of ltPTgt show a system size
    dependence with a maximum for peripheral PbPb
    collisions.
  • Similar dependence is found for the scaled
    variance of the multiplicity
  • of neg. charged particles (possible
    correlation ltPTgt - multiplicity).
  • Measurements of fluctuations of the net electric
    charge do not show
  • a reduction as had been proposed for
    QGP production .
  • The range of charge correlations (BF) decreases
    in central PbPb
  • collisions. The degree of reduction
    exhibits a smooth energy
  • dependence
  • Further experimental studies
  • Identify fluctuation signals of the onset of
    deconfinement
  • Search for the existence of the critical point
    of QCD.
  • LoI NA49-future Collaboration
  • CERN-SPSC-2006-001,CERN-SPSC-235
  • Study of hadron production in
    collisions of protons and nuclei

28
The NA49 collaboration
29
BACK UP
30
Event-by-Event estimationof the particle ratios
One Event
Event Ensemble
ltdE/dxgt
ltdE/dxgt
log(ptot GeV)
log(ptot GeV)


31
Extracting the Fluctuation Signal
Process the relative widths of the distributions
32
Net Charge Fluctuations Energy dependence
  • The predicted large suppression of the net-charge
    fluctuations is not observed!

33
Charge Correlations -The Balance Function
  • The Balance function is defined as a
    correlation in y of oppositely charged particles,
    minus the correlation of same charged particles,
    normalized to the total number of particles.

34
vsNN 8.8 GeV RAPIDITY DEPENDENCE
35
Rapidity dependence - vsNN 17.2 GeV
36
Energy dependence of average transverse mass
  • Increase of for final state
    particles (p,?,p)
  • slows sharply at the lowest SPS
    energy

37
Energy dependence pion yields
  • Increase of ratio with energy
  • gets steeper in the SPS range
  • Pion deficit changes to enhancement compared to
    pp
  • SMES statistical model of the
  • early stage

Increase of initial d.o.f. between AGS and SPS
38
Energy dependence ratio of strange hadrons to
pions
  • Strangeness to pion ratio peaks
  • sharply at the SPS
  • The peak is not seen in pp
  • collisions
  • SMES reproduces the data
  • Suggests ONSET of
  • deconfinement at SPS

39
Rapidity Spectra
40
Global view Phase diagram
Statistical model describes yields from AGS to
RHIC energies T of hadrochemical freeze out
increases
decreases
hadrochemical freeze out points at SPS energies
approach the phase boundary
41
Energy dependence of antibaryon/baryon ratios
The effect of the increasing baryon density is
seen in the strong decrease of antibaryon/baryon
ratios towards lower SPS energies.
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