Elliptic flow describes the azimuthalmomentum spaceanisotropy of particle emission from non-central heavy-ion collisions in the plane transverse to the beam direction, and is defined as the second harmonic coefficient of the azimuthal Fourier decomposition of the momentum distribution.[4] Elliptic flow is a fundamental observable since it directly reflects the initial spatial anisotropy, of the nuclear overlap region in the transverse plane, directly translated into the observed momentum distribution of identified particles. Since the spatial anisotropy is largest at the beginning of the evolution, elliptic flow is especially sensitive to the early stages of system evolution.[5] A measurement of elliptic flow thus provides access to the fundamental thermalization time scale and many more things in the early stages of a relativistic heavy-ion collision.[4]
^Voloshin, S.; Zhang, Y. (1996). "Flow study in relativistic nuclear collisions by Fourier expansion of azimuthal particle distributions". Zeitschrift für Physik C. 70 (4): 665–672. arXiv:hep-ph/9407282. doi:10.1007/s002880050141. S2CID118925144.