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Event -by- Event Physics at SPS Energies. P. Christakoglou, A. Petridis † , M. Vassiliou Athens University HEP2007 - Workshop Athens - March 2007. Outline. Introduction Energy - Centrality dependence of e-by-e fluctuations particle ratio

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event by event physics at sps energies
Event -by- Event Physics at SPS Energies

P. Christakoglou, A. Petridis†, M. Vassiliou

Athens University

HEP2007 - Workshop Athens - March 2007

outline
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
introduction
Introduction

Event-by-Eventmeasurements offer the possibility for studying the QGP phase transition and the nature of the QGP matter.

Pb+Pb 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.
the na49 detector

p > 7 GeV

dE/dx

forward rapidity

2,5 < p < 10 GeV :

TOF + dE/dx

at midrapidity

The NA49 Detector

Target: 20cm liquid H2 or Pb foil

VCAL detects projectile spectators

Δp/p2 = 7 (0.3) • 10-4 (GeV/c)-1

(VTPC-1, VTPC+MTPC)

dE/dx resolution 3 – 6 %

TOF resolution ~ 60 ps

particle ratio strangeness fluctuations
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 Κ/π 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 Pb+Pb collisions at all available beam energies.
acceptance
Acceptance

40 GeV:

160 GeV:

20 GeV:

the event by event k ratio
The Event-by-Event K/π ratio

Beam Energy

σ2dyn = σ2data – σ2mixed

the k ratio energy dependence
The K/π ratio – Energy dependence

Data : Increased fluctuation signal at lower beam energies

UrQMD: Κ/π fluctuation signal independent of beam energy

STAR

the event by event p p ratio
The Event-by-Event (p + p)/π ratio

Beam Energy

The distribution of the E-by-E p/π ratio is narrower for data than mixed events. Effect of baryon resonance decay ?

the p p ratio energy dependence
The (p + p)/π ratio – Energy dependence

NA49 preliminary

p/π fluctuation signal in UrQMD closely matches the energy dependence observed in the data

event by event fluctuations of p t
Event-by-event fluctuations of <pT>
  • 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

slide13

Event-by-event fluctuations of <pT>

1.1 < yπ < 2.6

  • distributions of <pT> similar
  • for real and mixed events
  • non-statistical (dynamical)
  • fluctuations are small, < few%
slide14

Centrality and Energy dependence

158A GeV

1.1 < yπ < 2.6

1.1 < yπ < 2.6

NA49 preliminary

increase for peripheral collisions, no increase at lower energy

multiplicity fluctuations
Multiplicity Fluctuations
  • Used measure of fluctuations: scaled variance

[ =1 for Poissonian distribution ]

  • 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
controlling centrality
Controlling Centrality

AProj

Veto Calorimeter

  • Veto calorimeter -> projectile spectators, number of projectile participants NPProj
  • Target spectators not measured in NA49

EVeto≈(AProj -NPProj)*Ekin

NPProj

multiplicity fluctuations1
Multiplicity Fluctuations

1.1 < y < 2.6

For non central Pb+Pb coll. the distributions are wider than the Poissonian one (independent particle production)

centrality dependence i
Centrality dependence (I)
  • Var(n)/<n> increases with decreasing centrality
  • Large fluctuations for peripheral collisions may be caused by equilibration (mixing) of particle sources from the projectile and target nuclei
results ii
Results II

Centrality dependence (II)

HSD, UrQMD:

V. Konchakovskyi et al.

Phys. Rev. C 73 (2006) 034902

HIJING:M. Gyulassy, X. N. Wang

Comput. Phys. Commun. 83 (1994) 307

Simulation performed by:M. Rybczynski

  • String hadronic models shown (UrQMD, HSD, HIJING) do not reproduce data on multiplicity fluctuations
net charge fluctuations
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 :
net charge fluctuations1
Net Charge Fluctuations

ΔΦq = Φq - Φq,gcc

QGP signature possibly erased by hadronisation (Bialas) or the effect of resonance decays (Zaranek)

charge correlations the balance function
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 δη quantified by the
  • balance function:

delayed hadronisation =

narrowing of balance function

predicted as signature of phase transition

system size and centrality dependence s nn 17 2 gev
System size and centrality dependence - √sNN = 17.2 GeV

The width takes its maximum value for p+p 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).

comparison na49 star

Au+Au@ √sNN = 130 GeV

J. Adams et al., (STAR Collaboration) Phys. Rev. Lett. 90, 172301 (2003)

Comparison NA49 – STAR

NA49 data show a strong centrality dependence of the orderof(17 ± 3)%.

STAR data show also a strong centrality dependence of the order of(14 ± 2)%.

slide25

Mid – rapidity (2.5 < η < 3.9)

Forward rapidity (4.0 < η < 5.4)

Rapidity dependence - √sNN = 17.2 GeV

conclusions
Conclusions

At the SPS the NA49 exp. has studied the e-by-e fluctuations:

  • The K/π ratio fluctuation signal increases at lower SPS energies.
  • The fluctuations of <PT> show a system size dependence with a maximum for peripheral Pb+Pb collisions.
  • Similar dependence is found for the scaled variance of the multiplicity

of neg. charged particles (possible correlation <PT> - 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 Pb+Pb

collisions. The degree of reduction exhibits a smooth energy

dependence

conclusions cont
Conclusions (cont.)

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

at the CERN SPS”

global view phase diagram
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

event by event estimation of the particle ratios

Vary relative normalization of the particle species (K/p,p/p) in the PDF

Fit dE/dx spectra in 4D binning

  • Extract ratios with maximum likelihood fit

Probability density function:

<dE/dx>

<dE/dx>

log(ptot [GeV])

Event-by-Event estimationof the particle ratios

One Event:

Event Ensemble:

<dE/dx>

<dE/dx>

log(ptot [GeV])

log(ptot [GeV])

extracting the fluctuation signal

Finite Number

Statistics

Experimental

Resolution

Dynamical

Fluctuations

“Data” Events

s = 23.27%

s = 15.9%

s = 16.7%

s = 2.8%

Events

Events

Events

Events

=

+

+

E-by-E K/p ratio

E-by-E K/p ratio

E-by-E K/p ratio

E-by-E K/p ratio

Statistical fluctuations

=

“mixed” Events

s = 23.1%

Events

E-by-E K/p ratio

Extracting the Fluctuation Signal

Process the relative widths of the distributions:

net charge fluctuations energy dependence
Net Charge Fluctuations Energy dependence
  • The predicted large suppression of the net-charge fluctuations is not observed!
charge correlations the balance function1

where P1: any rapidity interval in the detector

P2: relative rapidity interval

  • Bass-Danielewicz-Pratt, Phys.Rev.Lett.85, 2000
  • D. Drijard et al, Nucl. Phys. B(155), 1979
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.

s nn 8 8 gev rapidity dependence

Mid – rapidity(1.8 < η < 3.2)

Forward rapidity (3.3 < η < 4.7)

Acceptance filter OFF

Acceptance filter ON

√sNN = 8.8 GeV – RAPIDITY DEPENDENCE
rapidity dependence s nn 17 2 gev

Mid – rapidity (2.5 < η < 3.9)

Forward rapidity (4.0 < η < 5.4)

Acceptance filter OFF

Acceptance filter ON

Rapidity dependence - √sNN = 17.2 GeV
energy dependence of average transverse mass
Energy dependence of average transverse mass

Increase of for final state particles (π,Κ,p)

slows sharply at the lowest SPS energy

energy dependence pion yields
Energy dependence – pionyields
  • Increase of ratio with energy

gets steeper in the SPS range

  • Pion deficit changes to enhancement compared to p+p
  • SMES: statistical model of the

early stage

Increase of initial d.o.f.

between AGS and SPS

energy dependence ratio of strange hadrons to pions
Energy dependence – ratio of strange hadrons to pions
  • Strangeness to pion ratio peaks
  • sharply at the SPS
  • The peak is not seen in p+p
  • collisions
  • SMES reproduces the data
  • Suggests ONSET of
  • deconfinement at SPS
energy dependence of antibaryon baryon ratios
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.