What have we learned from Anisotropic Flow at RHIC ? - PowerPoint PPT Presentation

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What have we learned from Anisotropic Flow at RHIC ?

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Hiroshi Masui / University of Tsukuba. 7. Hadron identification. Time-of-flight ... Can we test these relations from the data ? ... – PowerPoint PPT presentation

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Title: What have we learned from Anisotropic Flow at RHIC ?


1
What have we learned from Anisotropic Flowat
RHIC ?
  • Hiroshi Masui
  • for the PHENIX Collaboration
  • 2006 RHIC AGS Annual Users meeting
  • June 5 9, 2006 at Brookhaven National
    Laboratory
  • Workshop 8 How perfect is this matter ?

2
Perfect liquid at RHIC
  • Strong collective flow, nearly perfect liquid

3
Definitions
Py
Pz
Z
Px
Reaction plane
Y
X
  • Anisotropic Flow
  • Azimuthal correlation to reaction plane
  • Elliptic flow (v2)

4
Outline
  • Elliptic Flow and Hydrodynamics
  • PHENIX experiment
  • Particle identification, event plane
  • Eccentricity scaling and speed of sound
  • Kinetic energy (Hydro) scaling and Partonic
    collectivity
  • Summary

5
v2 and hydrodynamics
PHENIX PRL 91, 182301 (2003)
D. Teaney PRC 68, 034913 (2003)
  • Large elliptic flow at RHIC
  • Elliptic flow is well described by hydrodynamics
  • Magnitude, particle type up to pT 1.5 GeV/c
  • Indicate early thermalization ? lt 1 fm/c,
    extremely low viscosity lt 0.1

6
PHENIX experiment
  • Hadron identification
  • Time-of-Flight
  • ? lt 0.35, ? lt ?/4
  • EM Calorimeter
  • ? lt 0.35, ? lt ?/2
  • Event plane
  • Beam Beam Counter, 3 lt ? lt 3.9, full azimuth

7
Hadron identification
  • Time-of-flight
  • ? lt ?/4, ? lt 0.35
  • Timing resolution 120 ps
  • ?/K separation 2 GeV/c
  • K/p separation 4 GeV/c
  • Good timing resolution
  • EM Calorimeter
  • ? lt ?/2, ? lt 0.35
  • Timing resolution 400 ps
  • ?/K separation 1 GeV/c
  • K/p separation 2 GeV/c
  • Large acceptance

8
Event plane _at_ 3lt?lt4
  • Large rapidity gap
  • Central arm ? lt 0.35 BBC 3 lt ? lt
    4
  • Smaller non-flow contribution

9
v2 from ideal fluid dynamics
cs 1/?3 t0 0.6 fm/c
b 8 fm
transverse size of system
R. S. Bhalerao, J.P. Blaizot, N. Borghini, J.-Y.
Ollitrault, PLB 627, 49, (2005)
  • v2 scales initial eccentricity (?)
  • v2/? is independent on system size R
  • v2 grows with cs
  • Can we test these relations from the data ?

10
Can we test eccentricity scaling of v2 ?
  • Does v2 scale eccentricity ?
  • Centrality dependence of v2/?
  • Is v2/? independent of system size ?
  • AuAu vs CuCu
  • Estimate of speed of sound can be made from the
    measurement of v2/?

11
Eccentricity and integrated v2
  • Eccentricity is usually estimated by Glauber
    Model
  • Integrated v2 is proportional to eccentricity
  • Advantage of integrated v2
  • Reduce large systematic error from Glauber MC,
    typically 20 30
  • Cancel systematic error from event plane
    determination

12
Eccentricity scaling
PHENIX PRELIMINARY
k 3.1 obtained from data
  • Scaling holds for a broad range of centrality
  • Centrality 30 -40 , b 8.7 fm
  • Independent of system size

13
Estimate of cs
v2/? _at_ ltpTgt 0.45 GeV/c
NOTE v2 value is typically factor 2 lager than
  • Cs 0.35 ? 0.05
  • Indicate softer EOS compared to cs1/?3
  • v2/? 0.1 (peripheral) 0.2 (central) at STAR
    and PHOBOS
  • Integrated v2 does not develop so much in the
    late hadronic stage

14
Kinetic energy scaling
M. Issah, A. Taranenko, nucl-ex/0604011
K0S, ? (STAR) PRL 92, 052302 (2004) ? (STAR)
PRL 95, 122301 (2005) ?, K, p (PHENIX)
preliminary
Meson v2
Baryon v2
Kinetic energy of a particle in a relativistic
fulid KET mT m0 at y 0
Hadron mass
  • Kinetic energy scaling works up to KET 1 GeV
  • Indicate hydrodynamic behavior
  • Possible hint of quark degrees of freedom at
    higher KET

15
What can we learn from identified hadrons ?
  • NCQ (Number of Constituent Quark) scaling of v2
    indicate partonic collectivity at RHIC
  • ? meson is a good probe to test NCQ scaling
  • No re-scattering in hadronic stage
  • Longer life time 40 fm/c
  • Thermal s-quark coalesce/recombine to form ? meson

QM2005, M. Oldenburg, STAR
16
Clear ? signal
  • ? ? KK-
  • Typical S/N 0.3
  • Centrality 20 60
  • S/N is good
  • Event plane resolution is good
  • Separation of v2 between meson and baryon is good
  • Magnitude of v2 do not vary very much

Before subtraction
Signal Background
Background
After subtraction
17
? Meson v2
N. Borghini, J.-Y. Ollitrault, PRC 70, 064905
(2004)
  • Obtained from invariant mass fit method
  • Consistent with standard subtraction method
  • Smaller systematic error
  • pT lt 2 GeV/c
  • Consistent with mass ordering from hydrodynamics

18
Partonic Collectivity (i)
Hydro. (KET) scaling
Hydro. Nquark scaling
SQM2006, S. Blyth, STAR
  • Hydro NCQ scaling works for ? meson
  • STAR result favors NCQ2 for ?
  • Consistent with other multi-strange hadrons (?,
    ?) from STAR
  • ? Collective flow of s-quark

19
Partonic Collectivity (ii)
PHENIX PRELIMINARY
WWND 2006, M. Issah
SQM2006, S. Esumi
Data QM2005, PHENIX
K0S, ? (STAR) PR 92, 052302 (2004) ? (STAR)
PRL 95, 122301 (2005) ? (STAR) preliminary
STAR preliminary 0-80 AuAu 200GeV Yan Lu
SQM05 P. Sorensen SQM05 M. Oldenburg QM05
K0S ? ? ?
  • Hydro NCQ scaling describes v2 for a variety of
    particles measured at RHIC
  • Scaling breaks for higher pT

20
Summary
  • What have we learned from anisotropic flow
    hydrodynamics at RHIC ?
  • Strongly interacting partonic matter
  • Large v2 ? Early thermalization, ? lt 1 fm/c
  • v2 scales eccentricity, independent of system
    size (Au, Cu)
  • Estimated speed of sound 0.35 ? 0.05
  • Partonic Collectivity
  • Kinetic energy NCQ scaling works for a broad
    set of particles
  • What more can be learned ?
  • Centrality, energy dependence of v2
  • v4/(v2)2 as a probe for degree of thermalization
  • PHENIX talks in this session
  • 225 PM S. Sakai, heavy flavor electron v2
  • 420 PM J. Newby, HBT

21
Thank you
22
Back up
23
v2/?, STAR, PHOBOS
v2/?part
v2/?
CIPANP 2006, S. Voloshin, STAR QM2005, S. Manly,
PHOBOS
  • v2/? 0.1 0.2
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