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STUDY OF CHARGE CORRELATIONS

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Panos Christakoglou, Angelos Petridis, Maria Vassiliou. University of Athens. for the NA49 and ALICE ... Due to cooling the width falls with time (stherm) ... – PowerPoint PPT presentation

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Title: STUDY OF CHARGE CORRELATIONS


1
STUDY OF CHARGE CORRELATIONS USING THE BALANCE
FUNCTION Panos Christakoglou, Angelos Petridis,
Maria Vassiliou University of Athens for the NA49
and ALICE Collaborations
2
OUTLINE
  • Introduction
  • Motivation.
  • BF definition and basic properties.
  • BF for all charged particles
  • System size dependence for two SPS energies.
  • Comparison with STAR.
  • Rapidity dependence.
  • Energy dependence study for all the SPS energies.
  • BF for identified particles
  • Preliminary results on the rapidity correlations.
  • Comparison with STAR.
  • Preliminary results on the momentum
    correlations.
  • Model calculations and predictions.
  • Extension of the method to LHC energies.
  • Summary.

3
OUTLINE
  • Introduction
  • Motivation.
  • BF definition and basic properties.
  • BF for all charged particles
  • System size dependence for two SPS energies.
  • Comparison with STAR.
  • Rapidity dependence.
  • Energy dependence study for all the SPS energies.
  • BF for identified particles
  • Preliminary results on the rapidity correlations.
  • Comparison with STAR.
  • Preliminary results on the momentum
    correlations.
  • Model calculations and predictions.
  • Extension of the method to LHC energies.
  • Summary.

4
MOTIVATION
  • Oppositely charged particles are created at the
    same location of space-time.
  • Charge - anticharge particles that were created
    earlier (early stage hadronization) are
    separated further in rapidity.
  • Particles pairs that were created later (late
    stage hadronization) are correlated at small ?y.
  • The Balance Function quantifies the degree of
    this separation and relates it with the time of
    hadronization.

5
DEFINITION
  • The Balance function is defined as a
    correlation in y of oppositely charge particles,
    minus the correlation of same charged particles,
    normalized to the total number of particles.

P1 any rapidity interval in the detector P2
relative rapidity difference
6
BALANCE FUNCTIONS HOW DO THEY WORK
  • The Balance Function is constructed in such way
    that can identify correlated pairs of oppositely
    charged particles on a statistical basis.

The numerator counts the pairs that satisfy both
criteria within an event and then is summed over
all events. The denominator counts particles that
were used for the creation of pairs within an
event and then summed over all events.
7
THE WIDTH OF THE BALANCE FUNCTION
  • The overall width of the Balance Function (BF) in
    relative rapidity is a combination of the thermal
    spread and the effect of diffusion.
  • Due to cooling the width falls with time
    (stherm).
  • The effect of diffusion stretches the BF (sdn).
  • If the hadronization occurred at early times then
    the effect of collisions is to broaden the BF.
  • On the other hand late stage hadronization would
    result into narrower BF.

8
OUTLINE
  • Introduction
  • Motivation.
  • BF definition and basic properties.
  • BF for all charged particles
  • System size dependence for two SPS energies.
  • Comparison with STAR.
  • Rapidity dependence.
  • Energy dependence study for all the SPS energies.
  • BF for identified particles
  • Preliminary results on the rapidity correlations.
  • Comparison with STAR.
  • Preliminary results on the momentum
    correlations.
  • Model calculations and predictions.
  • Extension of the method to LHC energies.
  • Summary.

9
SYSTEM SIZE DEPENDENCE - vsNN 17.3 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).
10
COMPARISON NA49 STAR
  • NA49 data show a decrease of the width of the
    order of (17 3) from the most peripheral to
    the most central PbPb collisions.
  • STAR data show also a strong centrality
    dependence of the order of (14 2).

STAR ? lt 1.3 NA49 -0.4lt?lt2.0
11
RAPIDITY DEPENDENCE _at_ SPS
The narrowing of the BF with centrality is
observed only in the mid-rapidity region.
P. Christakoglou et al. NA49 collaboration, AIP
Conf.Proc. 828, 107-112 (2006)
12
ENERGY DEPENDENCE _at_ SPS
  • First indication of an energy dependence for real
    data.
  • This dependence is not apparent in microscopic
    models such as UrQMD and HSD.

13
COMPARISON NA49 STAR
The results are not directly comparable yet,
since STAR studies the BF in a different phase
space window!!!
P. Christakoglou et al. NA49 collaboration, AIP
Conf.Proc. 828, 107-112 (2006)
14
ENERGY DEPENDENCE _at_ SPS FORWARD RAPIDITY
  • Motivated by the previous study, we have also
    analyzed the BF in the forward rapidity regions
    for each SPS energy.
  • Results show no energy dependence in the forward
    rapidity regions.
  • Interesting and important results for
    interpretations of the energy dependence.

15
OUTLINE
  • Introduction
  • Motivation.
  • BF definition and basic properties.
  • BF for all charged particles
  • System size dependence for two SPS energies.
  • Comparison with STAR.
  • Rapidity dependence.
  • Energy dependence study for all the SPS energies.
  • BF for identified particles
  • Preliminary results on the rapidity correlations.
  • Comparison with STAR.
  • Preliminary results on the momentum
    correlations.
  • Model calculations and predictions.
  • Extension of the method to LHC energies.
  • Summary.

16
SYSTEM SIZE DEPENDENCE PIONS
  • Width is extracted by calculating the weighted
    average in all the analyzed interval except the
    first bin (0.1-gt1.4).
  • This was done in order to exclude short range
    correlation effects, such as HBT or Coulomb, that
    are reflected in the first bin of the BF's
    distributions.
  • Width decreases with increasing system size and
    centrality for real data but not for the UrQMD
    points.

17
SYSTEM SIZE DEPENDENCE KAONS
  • Width is extracted by calculating the weighted
    average in all the analyzed interval exept the
    first bin (0.1-gt1.4).
  • No apparent sign of any centrality dependence in
    neither data nor UrQMD points.
  • Width decreases when going from CC to the most
    peripheral PbPb interactions.

18
RAPIDITY CORRELATIONS STAR
  • According to G. Westfall et. Al, J.Phys.G30,
    S345-S349 (2004), STAR studied the BF for pp and
    AuAu collisions at vs 200 GeV for different
    particle species.
  • Width for pion pairs decreases with increasing
    centrality.
  • No such dependence for kaon pairs and HIJING.

19
INVARIANT MOMENTUM STUDY
  • According to Scott Pratt and Sen Cheng,
    Phys.Rev.C68, 014907 (2003), if one studies the
    BF in terms of the invariant relative momentum,
    one could get a clearer insight about the
    possible physics interpretation.
  • In terms of laboratory momenta P and q the
    different components are defined as follows

20
MOMENTUM CORRELATIONS - CENTRALITY
  • Width is extracted by the fitting function.
  • Width decreases with centrality for pion pairs.
  • Results are inconclusive for kaon pairs.
  • Results are still preliminary.

sGeV/c
sGeV/c
21
OUTLINE
  • Introduction
  • Motivation.
  • BF definition and basic properties.
  • BF for all charged particles
  • System size dependence for two SPS energies.
  • Comparison with STAR.
  • Rapidity dependence.
  • Energy dependence study for all the SPS energies.
  • BF for identified particles
  • Preliminary results on the rapidity correlations.
  • Comparison with STAR.
  • Preliminary results on the momentum
    correlations.
  • Model calculations and predictions.
  • Extension of the method to LHC energies.
  • Summary.

22
AMPT v-1.11
  • AMPT is a multi-phase transport model which
    contains a quark-parton phase before
    hadronization.
  • It consists of four main components
  • Spatial and momentum distributions of hard
    partons and soft string excitations are obtained
    from HIJING.
  • The parton cascade follow the ZPC model.
  • When parton interactions cease, they are
    recombined with their parent strings to form
    hadrons according to LUND string fragmentation
    mechanism.
  • The scatterings among resulting hadrons are
    described by the relativistic transport model
    ART.
  • I used this model to generate PbPb events _at_ vsNN
    17.3 GeV for different centrality classes.

Zi-Wei Lin et al., Phys.Rev.C72, 064901 (2005 )
23
DEPENDENCE ON THE FREEZE-OUT TIME
  • In order to study the relation between the BF and
    the time of hadronization, we use the event mean
    of particle freeze-out time.

PRELIMINARY
There is a clear dependence of the width on the
hadronization time. The decrease is of the order
of (12 3).
24
DEPENDENCE ON THE MULTIPLICITY
  • I also studied whether this is just a trivial
    multiplicity dependence effect.
  • Within the same centrality class, I divided the
    sample into several sub-samples according to the
    number of generated particles for each event.
  • The outcome is that the narrowing of the width
    can not be attributed to the increasing
    multiplicity.

PRELIMINARY
25
DATA MODELS COMPARISON
  • We have already reported the narrowing of the
    width of the BF with increasing centrality for
    experimental data.
  • This decrease is of the order of (17 3).

PRELIMINARY
  • Microscopic models such as UrQMD and HIJING cant
    reproduce this narrowing.
  • On the other hand, the multi-phase trasport model
    AMPT with the time evolution of the partons can
    qualititivelly reproduce this behavior.
  • The decrease is of the order of (12 3).

26
OUTLINE
  • Introduction
  • Motivation.
  • BF definition and basic properties.
  • BF for all charged particles
  • System size dependence for two SPS energies.
  • Comparison with STAR.
  • Rapidity dependence.
  • Energy dependence study for all the SPS energies.
  • BF for identified particles
  • Preliminary results on the rapidity correlations.
  • Comparison with STAR.
  • Preliminary results on the momentum
    correlations.
  • Model calculations and predictions.
  • Extension of the method to LHC energies.
  • Summary.

27
PSEUDORAPIDITY STUDY SYSTEMATIC ERRORS
  • The cuts on three parameters were varied and the
    corresponding width was calculated.
  • The parameters were chosen to be Vz, br, bz.
  • The pseudorapidity phase space analyzed was
    -1.0,1.0.

PYTHIA events
ALICE Collaboration, Physics Performance Report
vII, CERN/LHCC/2005-030
28
PSEUDORAPIDITY STUDY INTERVAL STUDY
  • The analyzed interval was varied starting from
    1.0 (-0.5,0.5) up to 2.0 (-1.0,1.0) with a
    step 0.2.

PYTHIA events
ALICE Collaboration, Physics Performance Report
vII, CERN/LHCC/2005-030
29
RAPIDITY STUDY
  • Interval analyzed ALICE central barrel
    acceptance.

PYTHIA events
According to S.A. Bass, P. Danielewicz, S. Pratt,
Phys. Rev. Lett. 85, 2689 (2000), heavier
particles are characterized by narrower BF
distributions
ALICE Collaboration, Physics Performance Report
vII, CERN/LHCC/2005-030
30
OUTLINE
  • Introduction
  • Motivation.
  • BF definition and basic properties.
  • BF for all charged particles
  • System size dependence for two SPS energies.
  • Comparison with STAR.
  • Rapidity dependence.
  • Energy dependence study for all the SPS energies.
  • BF for identified particles
  • Preliminary results on the rapidity correlations.
  • Comparison with STAR.
  • Preliminary results on the momentum
    correlations.
  • Model calculations and predictions.
  • Extension of the method to LHC energies.
  • Summary.

31
SUMMARY
  • The BF might give insight about the time of
    hadronization.
  • The BF has been studied for all charged
    particles
  • Results from both SPS and RHIC show a strong
    system size and centrality dependence which is
    not seen in microscopic models and shuffled
    events.
  • Results from SPS show that the narrowing of the
    BF is only observed around mid-rapidity.
  • The scan throughout all SPS energies show a first
    indication of an energy dependence of the
    normalized parameter W.
  • The BF has also been studied for identified pion
    and kaon pairs
  • Preliminary results on the study of rapidity
    correlations show that there is a system size
    dependence of the width for pion pairs but not
    for kaon pairs.
  • Similar behaviour has been reported by STAR.
  • Preliminary results on the study of momentum
    correlations show that there is a system size
    dependence of the width for pion pairs but not
    for kaon pairs.
  • The study of a multi-phase model which
    incorporates the time evolution of partons before
    their hadronization revealed a clear relation of
    the width of the BF with the time of
    hadronization.
  • Method has been extended to LHC energies and the
    corresponding results have been included in the
    PPR vII. Work is still ongoing.
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