Speaker
Salvatore Plumari
(University of Catania (Italy))
Description
Viscous hydrodynamics is commonly used to model the evolution of the matter created
in an ultra-relativistic heavy-ion collision. It provides a good description of transverse
momentum spectra and anisotropic flow. These observables, however, cannot be consistently
derived using viscous hydrodynamics alone, because they depend on the microscopic
interactions at freeze-out. We derive the ideal hydrodynamic limit and the first-order
viscous correction to anisotropic flow ( $v_2$ , $v_3$ and $v_4$ ) and momentum spectrum using a
transport calculation [1]. We find that the linear response coefficient to the initial anisotropy, $v_n(p_T)/\epsilon_n$ ,
depends little on n in the ideal hydrodynamic limit. The viscous correction to the spectrum
depends not only on the differential cross section, but also on the initial momentum
distribution. This dependence is not captured by standard second-order viscous hydrodynamics.
The viscous correction to anisotropic flow increases with $p_T$ in agreement with the recent
analytical solutions of viscous hydrodynamic [2].
[1] S. Plumari, G. L. Guardo, V. Greco, J.Y. Ollitrault, Nucl.Phys. A 941 (2015) 87-96.
[2] Y. Hatta, J. Noronha, G. Torrieri, B.W. Xiao, Phys.Rev. D 90 (2014) 7, 074026.
On behalf of collaboration: | NONE |
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Author
Salvatore Plumari
(University of Catania (Italy))
Co-authors
Dr
Giovanni Luca Guardo
(INFN-LNS)
Jean-Yves Ollitrault
(CNRS)
Vincenzo Greco
(University of Catania)