Azimuthal anisotropy: Transition from hydrodynamic flow to jet suppression

Measured second and fourth azimuthal anisotropy coefficients v{sub 2,4}(N{sub part},p{sub T}) are scaled with the initial eccentricity {var_epsilon}{sub 2,4}(N{sub part}) of the collision zone and studied as a function of the number of participants N{sub part} and the transverse momenta p{sub T}. Sc...

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Veröffentlicht in:Physical review. C, Nuclear physics Nuclear physics, 2010-09, Vol.82 (3), Article 034910
Hauptverfasser: Lacey, Roy A., Taranenko, A., Wei, R., Ajitanand, N. N., Alexander, J. M., Jia, J., Pak, R., Rischke, Dirk H., Teaney, D., Dusling, K.
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Sprache:eng
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Zusammenfassung:Measured second and fourth azimuthal anisotropy coefficients v{sub 2,4}(N{sub part},p{sub T}) are scaled with the initial eccentricity {var_epsilon}{sub 2,4}(N{sub part}) of the collision zone and studied as a function of the number of participants N{sub part} and the transverse momenta p{sub T}. Scaling violations are observed for p{sub T} {le} 3 GeV/c, consistent with a p{sub T}{sup 2} dependence of viscous corrections and a linear increase of the relaxation time with p{sub T}. These empirical viscous corrections to flow and the thermal distribution function at freeze-out constrain estimates of the specific viscosity and the freeze-out temperature for two different models for the initial collision geometry. The apparent viscous corrections exhibit a sharp maximum for p{sub T} {ge} 3 GeV/c, suggesting a breakdown of the hydrodynamic ansatz and the onset of a change from flow-driven to suppression-driven anisotropy.
ISSN:0556-2813
1089-490X
DOI:10.1103/PhysRevC.82.034910