Abstract

We present measurements of the elliptic ($\mathrm{v}_2$), triangular ($\mathrm{v}_3$) and quadrangular ($\mathrm{v}_4$) anisotropic azimuthal flow over a wide range of pseudorapidities ($-3.5< \eta < 5$). The measurements are performed with Pb-Pb collisions at $\sqrt{s_{\text{NN}}} = 2.76$ TeV using the ALICE detector at the Large Hadron Collider (LHC). The flow harmonics are obtained using two- and four-particle correlations from nine different centrality intervals covering central to peripheral collisions. We find that the shape of $\mathrm{v}_n(\eta)$ is largely independent of centrality for the flow harmonics $n=2-4$, however the higher harmonics fall off more steeply with increasing $|\eta|$. We assess the validity of extended longitudinal scaling of $\mathrm{v}_2$ by comparing to lower energy measurements, and find that the higher harmonic flow coefficients are proportional to the charged particle densities at larger pseudorapidities. Finally, we compare our measurements to both hydrodynamical and transport models, and find they both have challenges when it comes to describing our data.

Highlights

  • The main goal of the heavy-ion physics program at the Large Hadron Collider (LHC) is to study the quark–gluon plasma (QGP), a deconfined state of matter existing at extreme temperatures and energy-densities

  • Due to the changing overlap geometry, a strong centrality dependence of the elliptic flow is observed over the entire pseudorapidity range

  • The present analyses extends the measurements to a wider range of pseudorapidity

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Summary

Introduction

The main goal of the heavy-ion physics program at the Large Hadron Collider (LHC) is to study the quark–gluon plasma (QGP), a deconfined state of matter existing at extreme temperatures and energy-densities. The anisotropic flow develops from pressure gradients originating from the initial spatial geometry of a collision and is observed as a momentum anisotropy in the finalstate particles. It is usually described by flow harmonics, which are defined as the Fourier coefficients: vn = cos [n(φ − n)] , (1). The flow harmonics v1 to v6 have been studied extensively at RHIC [1,2,3,4,5,6,7] and the LHC [8,9,10,11,12,13,14,15,16,17]. The observed anisotropic flow is considered to be a strong indication of collectivity [18] and is described well by relativistic hydrodynamics [19]

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