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π(0) 在 Au+Au 碰撞中从 √(s(NN))=39 到 200 GeV 的抑制的演化。

Evolution of π(0) suppression in Au+Au collisions from √(s(NN))=39 to 200 GeV.

机构信息

University of Colorado, Boulder, Colorado 80309, USA.

出版信息

Phys Rev Lett. 2012 Oct 12;109(15):152301. doi: 10.1103/PhysRevLett.109.152301. Epub 2012 Oct 9.

Abstract

Neutral-pion π(0) spectra were measured at midrapidity (|y|<0.35) in Au+Au collisions at √(s(NN))=39 and 62.4 GeV and compared with earlier measurements at 200 GeV in a transverse-momentum range of 1<p(T)<10 GeV/c. The high-p(T) tail is well described by a power law in all cases, and the powers decrease significantly with decreasing center-of-mass energy. The change of powers is very similar to that observed in the corresponding spectra for p+p collisions. The nuclear modification factors (R(AA)) show significant suppression, with a distinct energy, centrality, and p(T) dependence. Above p(T)=7 GeV/c, R(AA) is similar for √(s(NN))=62.4 and 200 GeV at all centralities. Perturbative-quantum-chromodynamics calculations that describe R(AA) well at 200 GeV fail to describe the 39 GeV data, raising the possibility that, for the same p(T) region, the relative importance of initial-state effects and soft processes increases at lower energies. The p(T) range where π(0) spectra in central Au+Au collisions have the same power as in p+p collisions is ≈5 and 7 GeV/c for √(s(NN))=200 and 62.4 GeV, respectively. For the √(s(NN))=39 GeV data, it is not clear whether such a region is reached, and the x(T) dependence of the x(T)-scaling power-law exponent is very different from that observed in the √(s(NN))=62 and 200 GeV data, providing further evidence that initial-state effects and soft processes mask the in-medium suppression of hard-scattered partons to higher p(T) as the collision energy decreases.

摘要

在质心系能量为 $\sqrt{s_{NN}}=39$ 和 62.4GeV 的 Au+Au 碰撞中,在中心快度区($|y|\lt0.35$)测量了中性π介子 $\pi(0)$ 的谱,并与在 200GeV 下测量的结果进行了比较,测量范围为 1<p(T)<10GeV/c。在所有情况下,高 p(T) 尾部都很好地由幂律描述,随着质心系能量的降低,幂律指数显著减小。这种变化与在相应的 p+p 碰撞谱中观察到的变化非常相似。核修正因子($R_{AA}$)表现出显著的抑制,且具有明显的能量、中心度和 p(T)依赖性。在 p(T)>7GeV/c 以上,对于所有中心度,$R_{AA}$ 在 $\sqrt{s_{NN}}=62.4$GeV 和 200GeV 下是相似的。在 200GeV 下很好地描述了 $R_{AA}$ 的微扰量子色动力学计算未能描述 39GeV 的数据,这增加了这样一种可能性,即在相同的 p(T)区域,在较低的能量下,初始状态效应和软过程的相对重要性增加。在中心 Au+Au 碰撞中,$\pi(0)$ 谱与 p+p 碰撞具有相同幂的 p(T)范围分别约为 5 和 7GeV/c,对于 $\sqrt{s_{NN}}=200$ 和 62.4GeV。对于 $\sqrt{s_{NN}}=39$GeV 的数据,尚不清楚是否达到了这样的区域,并且 x(T) 标度幂律指数的 x(T)依赖性与在 $\sqrt{s_{NN}}=62$ 和 200GeV 数据中观察到的非常不同,这进一步表明,随着碰撞能量的降低,初始状态效应和软过程掩盖了硬散射部分子在更高 p(T)处的介质抑制。

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