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Transcript of New Results from Viscous Hydro + URQMD (VISHNU) International School for High Energy Nuclear...
New Results from Viscous Hydro + URQMD (VISHNU)
International School for High Energy Nuclear Collisions , Wuhan, Oct 31- Nov.5, 2011
References:
Supported by DOE
11/04/2011
QGP viscosity at RHIC and LHC energies
H. Song , S. Bass and U. Heinz, Phys. Rev. C83, 024912 (2011)H. Song, S. Bass, U. Heinz, T. Hirano and C. Shen, Phys. Rev. Lett. 106, 192301(2011) H. Song, S. Bass, U. Heinz, T. Hirano and C. Shen, Phys. Rev. C83, 054910(2011)
1H. Song, S. Bass, U. Heinz, Phys Rev. C83 054912(2011)
Huichao Song 宋慧超
QGP-the most perfect fluid in the world?BNL News, 2005
How perfect the QGP fluid is? 2
0)( xT
S.Bass
gpuupeT )()(
u
T
T
2
12
u
T
Tu
2
1)(
viscous hydrodynamics
)( p Input: “EOS”
3
0)( xT gpuupeT )()(
u
T
T
2
12
u
T
Tu
2
1)(
viscous hydrodynamics
)( p Input: “EOS”
4
0)( xT
S.Bass
gpuupeT )()(
u
T
T
2
12
u
T
Tu
2
1)(
pre-equilibrium dynamics + viscous hydro + hadron cascade
viscous hydrodynamics
Initial conditions + viscous hydro (QGP) + hadron cascade (HRG)
Initial conditions + viscous hydro (QGP & HRG) + final conditions
)( p Input: “EOS”
5
Viscous hydro: Shear viscosity & elliptic flow V2
20-25% v2 suppression
4
1
s
Elliptic flow v2
-V2 can be used to extract the QGP shear viscosity
-For an accurate extraction of QGP viscosity, one needs to control the theoretical uncertainties as well as precise exp data.
H. Song and U. Heinz, PRC08
6
...])2cos(),(21[2
12
3
bpvdpdyp
dN
ddpdyp
dN
pd
dNE
TTT
TT
(GeV)Tp0 1
~30%
Partially Chemical equil.
Ideal hydro
P. Huovinen 07
Hadronic effects on elliptic flow V2 hadronic dissipative effects
~30-50%
-These two HRG effects are not included in early viscous hydro calculations
T. Hirano 06
viscous hydro + hadron cascade (URQMD) hybrid approach
URQMD includes the partially chemical equilibrium nature & hadronic dissipative effects
7
viscous hydro vs.
viscous hydro + hadron cascade
8
viscous v2 suppression
s95p-PCE
v2 suppression increases from ~20% (min visc hydro) to ~30% (min visc hydro + URQMD)
viscous hydro (QGP) + URQMD (HRG)
viscous hydro (QGP & HRG)
ideal hydro (QGP & HRG)
H. Song, S. Bass & U. Heinz, PRC11
20% 30%
9
STAR DATA
~20% uncertainties in EXP V2
~100% uncertainties for the extracted QGP viscosity
V2 from different exp methods are affected by non-flow and fluctuations
~20%
Extracting QGP viscosity from RHIC data
EXP.
10
Ollitrault, Poskanzer & Voloshin, PRC09Corrected v2:
with assumptions on fluctuations and non flow, all corrected v2 in participant / reaction plan converge to unique curves
greatly reduces uncertainties from EXP data for the extracted s/
Corrected V2
Extracting QGP viscosity from RHIC data
EXP.
11
-initial conditions-EoS: s95p-PCE Huovinen & Petreczky10
-chemical composition of HRG -viscosity of HRG-bulk viscosity: <20%
Viscous Hydro + URQMD
Extracting QGP viscosity from RHIC data
Song & Heinz, PRC 09
Theoretical Modeling
12
Song, Bass & Heinz, PRC2011
-initial conditions
-chemical composition of HRG -viscosity of HRG-bulk viscosity: <20%
Viscous Hydro + URQMD initial conditions
- Glauber / KLN initializations
- Fluctuation effects
Constrained from dN/dy and spectra
- initial flow
),,(, 00 yxs
v2 is sensitive to the initial conditions
dydNSv /)/1(/2
-EoS: s95p-PCE Huovinen & Petreczky10
Extracting QGP viscosity from RHIC data
Song & Heinz, PRC 09
13
Song, Bass & Heinz, PRC2011
: : QGP viscosity dydNSv /)/1(/2
dydNSv /)/1(/2 is insensitive to initial conditions, but sensitive to the QGP
viscosity in viscous hydro +URQMD calculations
H. Song, S. Bass, U. Heinz, T. Hirano, and C. Shen, PRL2011
14
theoretical vs. experimental
dydNSv /)/1(/2
---QGP viscosity
Ollitrault, Poskanzer & Voloshin, PRC09
- Corrected V2 in participant plan
Exp. Corrected V2
in part. plan
dydNSv /)/1(/2
S, - Glauber / fKLN (part. plan)
- dN/dy : STAR data 08
15
QGP viscosity from dydNSv /)/1(/2
24.016.0/ s for MC-KLN initial conditions
for MC-Glauber initial conditions 16.008.0/ s
MC-KLN MC-Glauber(Part. Plan) (Part. Plan)
16H. Song, S. Bass, U. Heinz, T. Hirano, and C. Shen, PRL2011
QGP viscosity from dydNSv /)/1(/2
24.016.0/ s for MC-KLN initial conditions
for MC-Glauber initial conditions 16.008.0/ s
effects from bulk viscosity effects from initial flow
MC-KLN (Part. Plan) (Part. Plan)
MC-Glauber
17
-a nice fit for both pion and proton spectra, insensitive to QGP viscosity
H. Song, S. Bass, U. Heinz, T. Hirano, and C. Shen, PRC2011
18
24.016.0/ s for KLN initial condi.for Glauber initial condi.16.008.0/ s
-hit the lower-bound of extracted from (non flow effects) dydNSv /)/1(/2 s/ -fluctuating effects is reduced by comparing theory & EXP. /2v
22 /}2{ v
5-10%
20-30%
30-40%
40-50%
5-10%
20-30%
30-40%
40-50%
20-30%
30-40%
40-50%
20-30%
30-40%
40-50%
08.0/ s
16.0/ s
Glauber Glauber
KLN KLN
H.Song, S. Bass , U. Heinz, T. Hirano, and C. Shen, PRC2011
19
QGP viscosity at RHIC & LHC energies
20
-- H. Song, S. Bass, U. Heinz, PRC2011
ALICE collaboration arXiv:1011.3914[nucl-ex]
V2(PT) at RHIC and LHC
Assuming const. s/
16.0/ s Approximately fit STAR v2{4}, but over predict ALICE v2{4}
This is not aim for extracting QGP viscosity at LHC energy with reliable uncertainty estimates
21
Song, Bass & Heinz, PRC2011
V2(PT) at RHIC and LHC
Assuming const. s/
This is not aim for extracting QGP viscosity at LHC energy with reliable uncertainty estimates
16.0/ s Approximately fit STAR v2{4}, but over predict ALICE v2{4}
16.0/ s24.020.0/ s
RHIC:LHC:
22
Song, Bass & Heinz, PRC2011
Is QGP fluid more viscous at LHC ?
Weakly coupled QGP
Lattice results
Assuming const. s/
)2(16.0/ cc TTs )3(24.0/ cc TTs
RHIC:LHC:
?
23
Song, Bass & Heinz, PRC2011
Is QGP fluid more viscous at LHC ?
We do not have enough evidence from v2 and spectra alone
At this moment, it is an open issue on whether QGP fluid is more viscous or perfect in temperature region covered by LHC ! 24
Song, Bass & Heinz, PRC2011
A short summary- is sensitive to
Extraction from elliptic flow data using viscous hydro + UrQMD indicates:
)41(3/)41(1 ss/
s/2v
)4/1()21(/ s
-Relatively smaller uncertainties are from
-other possible observables may help to reduce these uncertainties ,
initial flow, bulk viscosity, single short hydro vs. e-by-e simulations …
photons, HBT radii, triangular flow …
-Relatively larger uncertainties are from initial geometry MC-Glauber: MC-KLN: )4/1()32(/ s
25
Similar averaged QGP viscosity at RHIC and LHC energies
s/
HBT
V2
Spectra
Other free inputs in the hybrid model
Photons
26
e-b-e hydro vs. single shot hydro
Event-by-event hydro produces
5% less v2/ecc than single-
shot hydro with smooth
averaged initial profile
Zhi & Heinz, preliminary results
27
24.016.0/ s for MC-KLN initial conditions
for MC-Glauber initial conditions 16.008.0/ s
initial flow, bulk viscosity and e-b-e hydro:cancelation among them each of them shifts v2 by a few percent
28
29
30
31
Thank You
32
Thank You
33
HBT radii
sideout RR /- is sensitive to the QGP viscosity
- HBT HELPS to constrain the QGP viscosity, together with other observables (V2 …)
S. Pratt QM09
with viscosity
without viscosity
- However, viscosity is only one of the many ingredients that affect HBT radii (Pratt QM09)
34
EM probes: Photons Pion spectra
-Viscous hardening of PT-spectra is stronger for photons than hadrons
K. Dusling, 0903
20 ~/T
pp
peff
Photon spectra
1
~sTpe
-Photon spectra MAY HELP to constrain the 2-d range of QGP viscosity & thermalization time, together with other observables (V2 …)
-However, earlier thermalization also leads to harder photon spectra (Dusling 0903)
35
Triangular flow & QGP viscosity
-triangular flow is sensitive to QGP shear viscosity
Schenke, Jeon & Gale,arXiv:1009.3244 [hep-ph]
36
Triangular flow & QGP viscosity
-triangular flow is sensitive to QGP shear viscosity
Schenke, Jeon & Gale,arXiv:1009.3244 [hep-ph]
-triangular flow may help us to eliminate the uncertainties from KLN and Glauber
Zhi & Heinz, preliminary results
2
3
MC-KLN
MC-Glauber
37
LHC
38
& initialization models dydNSv /)/1(/2 Glauber
S, from MC- glauber (smearing) with finite nucleon size
from MC- glauber with very small nucleon size (delta function)
S,
The slope of theoretical curves is un-favor the early MC-Glauber model (with delta fun. )
dydNSv /)/1(/2
(used by some EXP. Group )
(used by our theoretical Cal)
39
Uncertainties from bulk viscosity
fm/c120)/( s
1C3.1C
1C100C
N-S initialization Zero initialization
-with a critical slowing down , effects from bulk viscosity effects are much smaller than from shear viscosity
bulk viscosity influences V2 ~5% (N-S initial.) <4% (zero initial.)
Song & Heinz, 0909
s/uncertainties to ~20% (N-S initial.) <15% (zero initial.)
fm/c120)/( s
s/ s/
40