论文标题
高能核冲突中喷气事件的全球几何特性
The global geometrical property of jet events in high-energy nuclear collisions
论文作者
论文摘要
我们介绍了全球几何模式的介质修改的第一项理论研究,即横向球($ s _ {\ perp} $)分布在相对论重型离子碰撞中具有Parton Energy损失的喷气事件的分布。在我们的调查中,Powheg+Pythia被用来对P+P基线中的横向球进行准确描述,该横向球体将近代领先顺序(NLO)PQCD计算与匹配的Parton淋浴(PS)结合在一起。 Parton能量损失的线性玻尔兹曼传输(LBT)模型被实施以模拟喷气机的中等内进化。我们计算中央PB+PB碰撞碰撞中的事件横向横向球分布,并进行培养基修改。在小$ s _ {\ perp} $区域的横向球分布的增强,但与P+P参考相比,在A+A碰撞中观察到了$ s _ {\ perp} $区域的抑制,这表明在PB+PB中的JET事件的总体几何形状在PB中变得更加类似铅笔。我们证明,对于重型离子碰撞最终状态中有2架喷气式的事件,喷射淬火使几何形状具有中等诱导的Gluon辐射的球体。但是,对于$ \ ge 3 $ 〜Jets的事件,QCD介质中的Parton Energy损失导致事件由于降低喷射数而更像铅笔,在这种情况下,较少的能量喷射可能会损失其能量,然后从喷气式选拔运动运动学切割中掉下来。这两个效应相互抵消,最终导致相对于p+p中的重型离子碰撞中的码头事件更多。
We present the first theoretical study of medium modifications of the global geometrical pattern, i.e., transverse sphericity ($S_{\perp}$) distribution of jet events with parton energy loss in relativistic heavy-ion collisions. In our investigation, POWHEG+PYTHIA is employed to make an accurate description of transverse sphericity in the p+p baseline, which combines the next-to-leading order (NLO) pQCD calculations with the matched parton shower (PS). The Linear Boltzmann Transport (LBT) model of the parton energy loss is implemented to simulate the in-medium evolution of jets. We calculate the event normalized transverse sphericity distribution in central Pb+Pb collisions at the LHC, and give its medium modifications. An enhancement of transverse sphericity distribution at small $S_{\perp}$ region but a suppression at large $S_{\perp}$ region are observed in A+A collisions as compared to their p+p references, which indicates that in overall the geometry of jet events in Pb+Pb becomes more pencil-like. We demonstrate that for events with 2 jets in the final-state of heavy-ion collisions, the jet quenching makes the geometry more sphere-like with medium-induced gluon radiation. However, for events with $\ge 3$~jets, parton energy loss in the QCD medium leads to the events more pencil-like due to jet number reduction, where less energetic jets may lose their energies and then fall off the jet selection kinematic cut. These two effects offset each other and in the end result in more jetty events in heavy-ion collisions relative to that in p+p.