Hydrodynamic afterburner for the color glass condensate and the parton energy loss - Hirano, Tetsufumi et al. Hydrodynamic description of ultrarelativistic heavy ion collisions - Kolb, Peter F. Relativistic viscous hydrodynamics, conformal invariance, and holography - Baier, Rudolf et al.
JHEP arXiv Second order hydrodynamic coefficients from kinetic theory - York, Mark Abraao et al. D79 arXiv From kinetic theory to dissipative fluid dynamics - Betz, B. The Applicability of causal dissipative hydrodynamics to relativistic heavy ion collisions - Huovinen, Pasi et al. Multiplicity scaling in ideal and viscous hydrodynamics - Song, Huichao et al. C78 arXiv C78 , Erratum: Phys. Anisotropies in momentum space at finite Shear Viscosity in ultrarelativistic heavy-ion collisions - Greco, V. Thermalization of gluons in ultrarelativistic heavy ion collisions by including three-body interactions in a parton cascade - Xu, Zhe et al.
Elliptic flow in transport theory and hydrodynamics - Gombeaud, Clement et al. Glauber modeling in high energy nuclear collisions - Miller, Michael L. Collective phenomena in non-central nuclear collisions - Voloshin, Sergei A.
Direct emission of multiple strange baryons in ultrarelativistic heavy ion collisions from the phase boundary - Dumitru, A. QCD saturation and deuteron nucleus collisions - Kharzeev, Dmitri et al. Hadronic dissipative effects on elliptic flow in ultrarelativistic heavy-ion collisions - Hirano, Tetsufumi et al. The Eccentricity in heavy-ion collisions from color glass condensate initial conditions - Drescher, Hans-Joachim et al.
Universality of the saturation scale and the initial eccentricity in heavy ion collisions - Lappi, T. Effect of flow fluctuations and nonflow on elliptic flow methods - Ollitrault, Jean-Yves et al. C80 arXiv Eccentricity fluctuations and its possible effect on elliptic flow measurements - Miller, Mike et al.
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Elliptic flow in the Gaussian model of eccentricity fluctuations - Voloshin, Sergei A. Importance of correlations and fluctuations on the initial source eccentricity in high-energy nucleus-nucleus collisions - Alver, B. The model exhibits thermodynamic of liquid-gas-phase transition comprising of a nucleus at low temperature liquid phase nucleons at high temperature gas phase and intermediate mass fragments liquid-gas mixed phase.
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Anisotropic flow is a response to the anisotropies in the initial geometry of the system created in heavy-ion collisions. Principal component analysis PCA method was applied to study event-by-event flow fluctuations.
Relativistic viscous hydrodynamic equations were derived invoking the second law of thermodynamics where all the second-order transport coefficients were uniquely determined within a single framework. The hydrodynamic fluctuations propagate by diffusion over large space-times and can have measurable contribution on the two-particle correlations though these vanish on ensemble averaging.
The anisotropic hydrodynamics equations employed describe the full spatiotemporal evolution of the transverse temperature, spheroidal momentum-space anisotropy parameter, and the associated three-dimensional collective flow of the matter. The momentum-space anisotropy is also taken into account in the computation of the dilepton production rate, allowing for a self-consistent description of dilepton production from the quark-gluon plasma. For our final results, we present predictions for high-energy dilepton yields as a function of invariant mass, transverse momentum, and pair rapidity.
We demonstrate that high-energy dilepton production is extremely sensitive to the assumed level of initial momentum-space anisotropy of the quark-gluon plasma. As a result, it may be possible to experimentally constrain the early-time momentum-space anisotropy of the quark-gluon plasma generated in relativistic heavy-ion collisions using high-energy dilepton yields. Radoslaw Ryblewski The H.
Library subscriptions will be modified accordingly. This arrangement will initially last for two years, up to the end of The dilepton emission rate as a function of transverse momentum left , invariant mass center , and rapidity right. Same as Fig. Same as the bottom panel of Fig.