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arXiv 0801.4545nucl-ex
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sqrt(s_NN)=200 GeV Au+Au碰撞中的双强子方位角关联

Dihadron azimuthal correlations in Au+Au collisions at sqrt(s_NN)=200 GeV

PHENIX Collaboration, A. Adare

摘要:

本文给出了在sqrt(sNN)= 200 GeV的Au+Au碰撞中,来自双喷注的带电强子在宽范围的横动量(0.4 < pT < 10 GeV/c)和中心度(0-92%)选择下的方位角(Δ φ)关联。随着pT的增加,远离侧Delta phi分布从宽且相对平坦的形状演变为凹形状,然后演变为凸形状。与p+p数据的比较表明,远场分布可以分为以Delta phi ~ π为中心的部分抑制的头部区域和以Delta phi ~ π \pm 1:1为中心的增强的肩部区域。在头部区域的相关强子的pT谱向中心碰撞软化。肩部区域的光谱斜率与中心性和触发pT无关。近侧分布的属性也修改相对于那些在p + p碰撞,反映在三角洲phi和三角洲eta的射流形状的扩大,和增强的每触发产量。然而,这些修改似乎仅限于pT < 4 GeV/c,超过这个值,双强子对的形状和每次触发的产额都变得类似于p + p碰撞。这些观测结果表明,无论是远离和近侧的分布包含喷流碎裂组件占主导地位的pT \ge 5 GeV和介质引起的组件,这是重要的pT \le 4 GeV/c。我们还量化的作用,在中间和低PT的射流通过产量的射流诱导对相比,二进制缩放p + p对产量。喷注诱导的对的产量被抑制在高对代理能量(两个强子的pT幅度的总和),并在低对代理能量增强。前者是一致的喷流淬火,后者是一致的软强子对由于运输损失的能量,以降低pT的增强。

英文摘要:

Azimuthal angle (Delta phi) correlations are presented for a broad range of transverse momentum (0.4 < pT < 10 GeV/c) and centrality (0-92%) selections for charged hadrons from di-jets in Au+Au collisions at sqrt(s_NN) = 200 GeV. With increasing pT, the away-side Delta phi distribution evolves from a broad and relatively flat shape to a concave shape, then to a convex shape. Comparisons to p+p data suggest that the away-side distribution can be divided into a partially suppressed head region centered at Delta phi ~ π, and an enhanced shoulder region centered at Delta phi ~ π\pm 1:1. The pT spectrum for the associated hadrons in the head region softens toward central collisions. The spectral slope for the shoulder region is independent of centrality and trigger pT . The properties of the near-side distributions are also modified relative to those in p + p collisions, reflected by the broadening of the jet shape in Delta phi and Delta eta, and an enhancement of the per-trigger yield. However, these modifications seem to be limited to pT < 4 GeV/c, above which both the dihadron pair shape and per-trigger yield become similar to p + p collisions. These observations suggest that both the away- and near-side distributions contain a jet fragmentation component which dominates for pT \ge 5GeV and a medium-induced component which is important for pT \le 4 GeV/c. We also quantify the role of jets at intermediate and low pT through the yield of jet-induced pairs in comparison to binary scaled p + p pair yield. The yield of jet-induced pairs is suppressed at high pair proxy energy (sum of the pT magnitudes of the two hadrons) and is enhanced at low pair proxy energy. The former is consistent with jet quenching; the latter is consistent with the enhancement of soft hadron pairs due to transport of lost energy to lower pT.

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