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Introduction to Viscous hydrodynamics

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Title: Introduction to Viscous hydrodynamics


1
Viscous hydrodynamics for relativistic heavy-ion
collisions
Huichao Song
Department of Physics
The Ohio State University
191 West Woodruff Avenue
Columbus, OH 43210
2007 National Nuclear Summer School
FSU, FL. July 8 July 21, 2007
Advisor U. Heinz, Supported by DOE
2
The QCD Phase Diagram
QGP
3
The QGP Shear Viscosity
The QGP shear viscosity of is in hot theoretical
debates recently
-Weakly coupled QCD prediction
P.Arnold,G.Moore,Y.Yaffe, 00,03
-Strongly coupled AdS/CFT prediction
D.T. Son, et,al. 03
The first estimation of the QGP shear viscosity
from the experimental data (RHIC)
--blast wave model the first order theory
corrections
D. Teaney, PRC 68 (2003) 034913
Blast wave model analysis
-only counts the viscous corrections to the
spectra during freeze-out procedure
-neglects shear viscosity effects on hydro
dynamic evolution before freeze-out
Viscous hydrodynamics is needed!
4
Ideal hydrodynamics

hydro
S.Bass
Hydrodynamics
-A macroscopic tool to describe the expansion of
QGP or hadronic matter
Conservation laws
5 equ. 14 independent variables
-reduce of independent variables (ideal hydro)
-Provide more equations? (viscous hydro)
Ideal hydrodynamics reduce the independent
variable from 14 to 6,
5
Causal viscous hydrodynamics
Full tensor decomposition in frame of
Besides these modified transport equations for
, one need more equations
for these dissipative flows
The first order theory formulism
--- Eckart, Landau Lifishitz around 1950s
Problems in the first order theory formulism
-Acuasl, infinite speed of signal propagation
-process instabilities
6
Causal viscous hydrodynamics
Full tensor decomposition in frame of
W. Israel, J.Stewart 79
The 2nd order Israel-Stewart formulation
--expansion the entropy current to the 2nd order
of dissipative flows,
7
Causal viscous hydro in (21)-d
U. Heinz, H. Song A. Chaudhuri, PRC 73(2006)
034904
31 21
-zero net baryon density, zero bulk pressure,
zero heat conduction
Equivalent to the modified transport equations
for
where, the transport equations for energy
momentum tensor are explicit written as
8
Viscous vs. ideal hydro temperature entropy
-slowing down of cooling process due to
decelerated longitudinal expansion initially ,
but faster cooling in middle and late stages due
to stronger transverse expansion
-viscous effects are larger in early and middle
stages, but neglectable in late stage
9
Viscous vs. ideal hydro radial flow spectra
-More radial flow, flatter spectra
-the viscous effects to the hadron spectra could
be absorbed by starting viscous
hydro later with lower initial energy density
10
Viscous vs. ideal hydro elliptical flow
For non-central collisions
-Elliptical flow is very sensitive to even
minimal shear viscosity.
11
Summery and Conclusions
- Shear viscosity results in slowing down of the
cooling process in early stage due
to decelerated longitudinal expansion, faster
cooling in middle and late stages due
to stronger transverse expansion.
-Shear viscosity leads to more radial flow
generation and flatter spectra, the effects
of which could be absorbed by starting viscous
hydro later with lower initial energy
density.
-elliptical flow is very sensitive to shear
viscosity, even the minimum value from
AdS/CFT could result in a great suppression of
.
  • in contrast with the Teaneys blast wave model
    method, which only counts viscous

spectra corrections during freeze-out
procedure, our results shows that evolution
  • corrections ( ) are the main factor to
    influence the low spectra elliptical flow.

-Do the results indicate that the QGP viscosity
smaller than the AdS/CFT lowest
limit? Need more investigations in the at
least flowing aspects
a)Different initial conditions
b) more realistic descriptions of the hadronic
stage
12
Thank You
13
1st order theory vs. 2nd order theory
As the relaxation time reduces to zero, the 2nd
order theory formulism returns to the 1st order
one. First order theory ,
instable ?
a) calculated with the same velocity
profile from the 2nd theory by

not the real 1st order Navier-Stokes hydrodynamics
b)Smaller relaxation time reduces the viscous
effects on suppression of
14
Blast wave model vs. real viscous hydrodynamics
Blast wave model
viscous hydrodynamics
vs.
the1st order theory corrections
(the 2 order theory Israel-Stewart formulation)
--with both evolution and spectra corrections
--with only spectra corrections
Compare the spectra corrections from blast wave
model and from real hydrodynamics
-Spectra corrections are sensitive to the details
of flow pattern at freeze out, and are
not easily captured with blast-wave model
parametrizations.
15
viscous vs. ideal hydro central CuCu
collisions
16
viscous vs. ideal hydro central CuCu
collisions
17
Viscous vs. ideal hydro momentum anisotropy
18
Where ideal hydro works
  • spectra for both central collision and
    noncentral collisions

Hydro U Heinz P.Kolb Data STAR PHENIX
19
Where ideal hydro works
  • Elliptic flow coefficient at noncentral
    collisions

STAR, PHENIX, PHOBOS
STAR PRL04 PHENIX PRL03
for different identified hadrons
as a function of centrality
-Ideal hydro describes the data well at
-It also gives a correct mass splitting of
at low region
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