Title: Event by Event Fluctuations in the NA49 Experiment
1Event -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
2Outline
- 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
-
3Introduction
- 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. -
4The 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
5PbPb collision at 158A GeV
6Particle 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.
7Acceptance
40 GeV
160 GeV
20 GeV
8The Event-by-Event K/p ratio
Beam Energy
s2dyn s2data s2mixed
9The K/p ratio Energy dependence
STAR
- Data Increased fluctuation signal at lower
beam energies - UrQMD ?/p fluctuation signal independent of beam
energy -
10The 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 ?
11The (p p)/p ratio Energy dependence
NA49 preliminary
p/p fluctuation signal in UrQMD closely matches
the energy dependence observed in the data
12Event-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
13Event-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
15Multiplicity 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
16Controlling 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
17Multiplicity Fluctuations
1.1 lt y lt 2.6
For non central PbPb coll. the distributions
are wider than the Poissonian one (independent
particle production)
18Centrality dependence (I)
- Var(n)/ltngt increases with decreasing centrality
- Approximate scaling in NPProj/AProj
19Results 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
20Net Charge Fluctuations
- Net charge fluctuations will be smaller in QGP
(due to fractional charges of quarks) than
in gas of hadrons - The Fluctuation Measure
-
21Net Charge Fluctuations
?Fq Fq - Fq,gcc
QGP signature possibly erased by hadronisation
(Bialas) or the effect of resonance decays
(Zaranek)
22Charge 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
23System 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).
24Comparison 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).
25Rapidity dependence - vsNN 17.2 GeV
26Energy dependence
27Conclusions
- 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
28The NA49 collaboration
29BACK UP
30Event-by-Event estimationof the particle ratios
One Event
Event Ensemble
ltdE/dxgt
ltdE/dxgt
log(ptot GeV)
log(ptot GeV)
31Extracting the Fluctuation Signal
Process the relative widths of the distributions
32Net Charge Fluctuations Energy dependence
- The predicted large suppression of the net-charge
fluctuations is not observed!
33Charge 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.
34vsNN 8.8 GeV RAPIDITY DEPENDENCE
35Rapidity dependence - vsNN 17.2 GeV
36Energy dependence of average transverse mass
- Increase of for final state
particles (p,?,p) - slows sharply at the lowest SPS
energy
37Energy 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
38Energy 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
39Rapidity Spectra
40Global 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
41Energy 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.