Relating eccentricity fluctuations to density fluctuations in heavy-ion collisions
arXiv:1903.06366 · doi:10.5506/APhysPolB.50.1165
Abstract
The magnitude of anisotropic flow in a nucleus-nucleus collision is determined by the energy density field, $Ï(x,y,z)$, created right after the collision occurs. Specifically, elliptic flow, $v_2$, and triangular flow, $v_3$, are proportional to the anisotropy coefficients $\varepsilon_2$ and $\varepsilon_3$, which are functionals of $Ï$. We express the mean and the variance of $\varepsilon_2$ and $\varepsilon_3$ as a function of the 1- and 2-point functions of $Ï$. These results generalize results obtained previously, that were valid only for central collisions, or only for identical point-like sources. We apply them to the color glass condensate effective theory, using the recently derived expression of the 2-point function.
12 pages, 2 figures. v2: minor changes in figures, acknowledgments added. Proceedings of XXV Epiphany conference on Advances in Heavy Ion Physics, Cracow, Poland, 8-11 January 2019