\documentclass{article} %\topmargin -2cm %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %\usepackage{graphicx}% Include figure files %\usepackage{dcolumn}% Align table columns on decimal point %\usepackage{bm}% bold math %\usepackage{color} \usepackage{lineno} \usepackage[numbers,sort&compress]{natbib} \usepackage[top=3.54cm, bottom=3.54cm, left=4.0cm,right=4.0cm]{geometry} %页面边距 %\usepackage[colorlinks, % bookmarks=true, % linkcolor=blue, % %pdfborder=blue? % urlcolor=blue, % anchorcolor=black, % citecolor=blue % ]{hyperref} %\usepackage[all]{hypcap} \newcommand {\rootsNN} {\ensuremath{\sqrt{s_{_{\rm{NN}}}}}} \begin{document} \begin{center} \textbf{\Large Onset of Partonic Collectivity in Heavy-Ion Collisions at RHIC }\\ \end{center} \begin{center} \textbf{Li-Ke Liu}\\ \textbf{(for the STAR Collaboration)}\\ \end{center} \begin{center} \end{center} \linenumbers Partonic collectivity is one of the key signatures for the formation of quark-gluon-plasma in high-energy nuclear collisions. Scaling with the number of constituent quarks (NCQ) of elliptic flow ($v_2$) has been observed at top RHIC energy ({\rootsNN} = 200 GeV) and at the LHC ({\rootsNN} = 2.76 TeV), indicating the presence of partonic collectivity. Meanwhile, NCQ scaling is absent for identified particles at {\rootsNN} = 3 GeV Au+Au collisions. In this talk, we present a systematic analysis of $v_2$ for light, strange, multi-strange, and $\phi$ mesons in Au+Au collisions at {\rootsNN} = 3.0, 3.2, 3.5, 3.9, 4.5, 7.7, 9.2, 11.5, 14.5, 17.3, and 19.6 GeV, using data from the STAR experiment at RHIC. While NCQ scaling is clearly violated at {\rootsNN} $\le$ 3.2 GeV, implying a hadronic interaction-dominated equation of state, the scaling is gradually restored as the energy increases up to the 4.5 GeV Au+Au collisions, indicating the onset of the partonic interactions in these collisions. The $v_2$ results of multi-strange hadrons and $\phi$ mesons, with new high statistics data, will be shown for collision energies {\rootsNN} $\ge$ 7.7 GeV. In addition, the energy dependence of the $p_T$-integrated $v_2$ for different particle species will be compared with predictions from transport model calculations. Finally, we will discuss the implications of these measurements on understanding of QCD phase structure. %\nolinenumbers \end{document}