Title: What have we learned from Anisotropic Flow at RHIC ?
1What 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 ?
2Perfect liquid at RHIC
- Strong collective flow, nearly perfect liquid
3Definitions
Py
Pz
Z
Px
Reaction plane
Y
X
- Anisotropic Flow
- Azimuthal correlation to reaction plane
- Elliptic flow (v2)
4Outline
- Elliptic Flow and Hydrodynamics
- PHENIX experiment
- Particle identification, event plane
- Eccentricity scaling and speed of sound
- Kinetic energy (Hydro) scaling and Partonic
collectivity - Summary
5v2 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
6PHENIX 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
7Hadron 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
8Event plane _at_ 3lt?lt4
- Large rapidity gap
- Central arm ? lt 0.35 BBC 3 lt ? lt
4 - Smaller non-flow contribution
9v2 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 ?
10Can 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/?
11Eccentricity 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
12Eccentricity 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
13Estimate 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
14Kinetic 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
15What 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
16Clear ? 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
18Partonic 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
19Partonic 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
20Summary
- 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
21Thank you
22Back up
23v2/?, STAR, PHOBOS
v2/?part
v2/?
CIPANP 2006, S. Voloshin, STAR QM2005, S. Manly,
PHOBOS