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FIAS Scientific Report 2011 - Frankfurt Institute for Advanced Studies ...

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Effects of temperature dependent shear viscosity over the entropy density ratio on elliptic flow<br />

in ultrarelativistic heavy-ion collisions<br />

Collaborators: G.S. Denicol 1 , P. Huovinen 1 , E. Molnár 2,3 , H. Niemi 2,4 , D.H. Rischke 1,2<br />

1 Institut für Theoretische Physik, Johann Wolfgang Goethe-Universität, 2 <strong>Frankfurt</strong> <strong>Institute</strong> <strong>for</strong> <strong>Advanced</strong> <strong>Studies</strong>, 3 MTA<br />

Wigner Research Centre <strong>for</strong> Physics, Budapest, Hungary, 4 Department of Physics, University of Jyväskylä, Finland<br />

Presently, most hydrodynamical models of ultrarelativistic heavy-ion collisions assume a constant, temperatureindependent<br />

shear viscosity to entropy ratio η/s. In several works it has been claimed that in order to describe<br />

elliptic flow data, this constant value cannot be significantly larger than the lower bound η/s = 1/4π conjectured<br />

in the framework of the AdS/CFT correspondence. A constant η/s is, however, in contrast to the typical<br />

behavior observed in common fluids, where η/s has a strong temperature dependence and, typically, a minimum<br />

near phase transitions. A similar behavior of η/s is expected <strong>for</strong> finite-temperature matter described<br />

by quantum chromodynamics (QCD) near the transition from hadronic matter to the QGP (the QCD phase<br />

transition). We have investigated a question, whether the temperature dependence of η/s has an effect on the<br />

collective flow of hadrons in heavy-ion collisions.<br />

In Au+Au collisions at RHIC, we find almost no difference in elliptic flow whether η/s is constant in the QGP<br />

phase or strongly increasing with temperature. In contrast, the elliptic flow is highly sensitive to the values of<br />

η/s in the low-temperature hadronic phase. On the other hand, we found that the sensitivity of the elliptic flow<br />

to the values of η/s in the high-temperature QGP increases with increasing collision energy, while the effect<br />

of the hadronic viscosity decreases. At the highest LHC energy, the above conclusion <strong>for</strong> RHIC energies is<br />

reversed: suppression of the elliptic flow is dominated by the viscosity of the QGP and insensitive to that of the<br />

hadronic phase.<br />

The insensitivity of the elliptic flow to the high-temperature shear viscosity in Au+Au collisions at RHIC is<br />

illustrated in the Figure below, where our result from the hydrodynamical simulations are compared with the<br />

data from the STAR Collaboration.<br />

η/s<br />

1.2<br />

1.0<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

LH-LQ<br />

LH-HQ<br />

HH-LQ<br />

HH-HQ<br />

0.0<br />

0.10 0.20 0.30 0.40<br />

T [GeV]<br />

v 2 (p T )<br />

0.2<br />

0.1<br />

STAR v 2 {4}<br />

20-30 %<br />

0.0<br />

charged hadrons<br />

RHIC 200 AGeV<br />

0 1 2<br />

pT [GeV]<br />

3<br />

Left: The parametrizations of η/s as a function of temperature Right: Elliptic flow of charged hadrons in 20-30 %<br />

centrality class in Au+Au collisions at RHIC. The data is 4-particle cumulant data from the STAR Collaboration<br />

Related publications in <strong>2011</strong>:<br />

1) H. Niemi, G. S. Denicol, P. Huovinen, E. Molnar and D. H. Rischke, Influence of the shear viscosity of<br />

the quark-gluon plasma on elliptic flow in ultrarelativistic heavy-ion collisions, Phys. Rev. Lett. 106 (<strong>2011</strong>)<br />

212302.<br />

40

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