Title: Elliptic Flow in PHENIX
1Elliptic Flow in PHENIX
- Hiroshi Masui
- for the PHENIX collaboration
- CIPANP 2006, Westin Rio Mar Beach
- Puerto Rico
- May 30 Jun 3, 2006
2Why Elliptic Flow ?
Z
- Study the properties of matter created at RHIC
- The probe for early time
- The dense nuclear overlap is ellipsoid at the
beginning of heavy ion collisions - Pressure gradient is largest in the shortest
direction of the ellipsoid - Spatial anisotropy ? Momentum anisotropy
- Signal is self-quenching with time
- Elliptic flow (v2) is defined by the 2nd
coefficient of Fourier expansion
Reaction plane
Y
X
Pz
Py
Px
3Outline
partonic
hadronic
?
direct?
Elliptic Flow, v2
time
D
?, K, p
Partonic degrees of freedom, Thermalization, ..
- Elliptic Flow, v2
- Bulk, early probe
- Charged hadrons
- give us a base line
- ? Meson
- Small interaction cross section, long lived life
time (40 fm/c) - Penetrating probes
- Heavy flavor electrons (charm)
- Direct ?
4Baseline charged hadrons
Charged hadrons, v2 vs pT
PHENIX PRL 91, 182301 (2003)
v2 k ? ?
- Large elliptic flow at RHIC
- Consistent with hydrodynamics with rapid
thermalization, ? 1 fm/c - v2 scales initial eccentricity (?) of reaction
zone
5Hydro scaling
M. Issah, A. Taranenko, nucl-ex/0604011
Hydro scaling of v2
K0S, ? (STAR) PRL 92, 052302 (2004) ? (STAR)
PRL 95, 122301 (2005) ?, K, p (PHENIX)
preliminary
Meson v2
Baryon v2
KET mT m0 at y 0
- Scaling holds up to KET 1 GeV
- Meson/Baryon v2
- Possible hint of partonic degrees of freedom
61. ? meson v2
7Clear ? signal
- ? reconstruction via KK- decay channel
- S/N 0.3
- Centrality 20 60
- S/N is good
- Event plane resolution is good
- Separation between meson/baryon v2 is good
- v2 do not be varied too much.
Before subtraction
Signal Background
Background
After subtraction
8Meson type flow !
? v2 vs pT
- Hydro. mass ordering for pT lt 2 GeV/c
- v2(?) v2(?), v2(K) for pT gt 2 GeV/c
- Mass Number of constituent quarks
- Consistent with the description by quark
coalescence, recombination models
9Hint of partonic d.o.f
Hydro scaling of v2
K0S, ? (STAR) PR 92, 052302 (2004) ? (STAR)
PRL 95, 122301 (2005) ? (STAR) preliminary ?,
K, p, ?0, d (PHENIX) preliminary
- Hydro Nquark scaling
- Works for a broad range of KET
- ? meson also follow the scaling
- Partonic degrees of
- freedom
WWND 2006, M. Issah
102. Heavy flavor electron v2
11Clean heavy flavor electron
Cocktail subtraction
Converter subtraction
Signal / Background ratio
Run4
Run2
- Two different techniques show an excess heavy
flavor electron signal - Signal/Background gt 1 for pT gt 1 GeV/c
12Hint of Charm flow
e v2 vs pT
V. Greco, C. M. Ko, R. Rapp PL B 595, 202 (2004)
- Data indicate finite v2 of charm quark
- Suggest thermalization of c quark as well as
light quarks - What is the origin of high pT drop ?
13b quark contribution ?
e v2 vs pT
H. Hees, V. Greco, R. Rapp PRC 73, 034913 (2006)
(1)
- D or B meson v2
- decrease, (2) flat at high pT
input
(2)
v2
D ? e
output
B ? e (1)
Simulation
B ? e (2)
SQM 2006, S. Sakai
pT (GeV/c)
- High pT drop might be explained by B meson
contribution
143. Direct ? v2
15Clear Direct ? signal
PRL 94, 232301 (2005)
- Large direct ? excess
- ?0 is suppressed but direct ? not
- Both results are consistent with pQCD
16Possible 3 different scenarios
? v2 vs pT
PRL 96, 032302 (2006)
- Direct ? v2
- 1. Hard scattering
- v2 0
- 2. Parton fragmentation
- v2 gt 0
- 3. Bremsstrahlung
- v2 lt 0
- Inclusive ?
- Consistent with expected ? v2 from hadron decays
17v2direct? 0 ?
? v2 vs pT
PRL 96, 032302 (2006)
- Direct ? v2
- Direct ? excess ratio is consistent with
v2BG/v2inclusive?, suggest v2direct? 0 - Favors prompt photon production for dominant
source of direct ?
18Conclusions
- Elliptic Flow is powerful tool to study hot and
dense matter at RHIC - ? meson ? Partonic degrees of freedom
- Hydro. mass ordering for pT lt 2 GeV/c
- For pT gt 2 GeV/c, v2(?) prefer quark composition
not mass - Hydro Nquark scaling works for ? meson as well
as other hadrons - Heavy flavor electron ? Thermalization
- Consistent with non-zero charm flow, suggest
thermalization of c quark as well as light quarks - Bottom contribution at high pT need to be studied
experimentally - Direct ? ? Coming soon
- v2direct? 0, consistent with the scenario of
direct ? production from initial hard scattering - Year-4 data may enable us to reduce statistical
error bars, and extend pT reach, and to measure
thermal ? v2
19Thank you
20Back up
21Converter Subtraction method
Ne
0.8
1.1
?
1.7
With converter
Photonic electron
W/o converter
Photon Converter (Brass 1.7 X0) around beam
pipe
Conversion from beam pipe
Dalitz 0.8 X0 equivalent
Non-photonic electron
0
X0
- Source of background electrons
- Photon conversion ?0 ? ? ? ? ee-
- Dalitz decay (?0 ?ee?, ? ?ee?, etc)
- Di-electron decays of ?, ?, ?
- Kaon decays
- Conversion of direct photons
22Inclusive electron v2 (w., w/o. converter)
- Converter subtraction method
- Inclusive electron v2 w. and w/o. converter.
- Clear difference between them.
- Electron v2 with converter include large photonic
component.
23Inclusive photonic electron v2
- Photonic electron v2
- pT lt 1 GeV/c
- ? Converter method
- pT gt 1 GeV/c
- Simulation
- v2(inclusive) lt v2 (photonic)
- ? v2(non-photonic) lt v2(photonic)
photonic e v2
inclusive e v2 (w/o. converter)
24Centrality dependence
- Non zero heavy flavor electron v2 !
25Run4 inclusive ? v2
?0
v2
inclusive ?
pT
26Independent on system size
Eccentricity scaling
- Eccentricity scaling
- A wide range of centrality
- Independent of system size
- Integrated v2 ? eccentricity
- Reduce systematic error from eccentricity
calculation - Cancel systematic error by the ratio of v2(pT) /
(integrated v2)
27Hadron identification
- Time-of-flight
- ? lt ?/4, ? lt 0.35
- Timing resolution 120 ps
- ?/K separation 2 GeV/c
- K/p separation 4 GeV/c
- EM Calorimeter
- ? lt ?/2, ? lt 0.35
- Timing resolution 400 ps
- ?/K separation 1 GeV/c
- K/p separation 2 GeV/c
28The PHENIX experiment
- Acceptance
- Central arm ?? lt ?, ?? lt 0.35
- Centrality
- Beam-Beam Counter, Zero Degree Calorimeter.
- Event plane
- BBC
- Tracking
- Drift chamber, Pad chambers.
- Particle identification
- Electron
- Electro-Magnetic Calorimeter
- Hadron
- Time-of-Flight, Aerogel Cherenkov Counter, EMCal