论文标题
流动分布的系统分析
Systematic Analysis of Flow Distributions
论文作者
论文摘要
从流动谐波分布和累积物中提取了事件波动的信息,可以通过实验完成。在这项工作中,我们使用正常内核采用了革兰氏阴性级别的标准方法来找到这种分布,这是对最近引入的流量分布的概括,以研究事件逐渐发生的波动。另外,我们介绍了一组新的累积物$ j_n \ {2k \} $,该$与其他已知累积物相比,具有更多有关波动的信息。 The experimental data imply that not only all of the information about the event-by-event fluctuations of collision zone properties and different stages of the heavy-ion process are not encoded in the radial flow distribution $p(v_n)$, but also the observables describing harmonic flows can generally be given by the joint distribution $\mathcal{P}(v_1,v_2,...)$.通过这种方式,我们首先引入一组关节累积剂$ \ MATHCAL {K} _ {nm} $,然后使用这些关节累积物找到流量接头分布。最后,我们表明,从爱丽丝数据获得的对称累积$ SC(2,3)$和$ SC(2,4)$由组合$ \ Mathcal {k} _ {22}+\ frac {1} {1} {1} {2} {2} {2} {k} _ {k} _ {04} $ {04} $ {k {k {k) $ \ MATHCAL {K} _ {22} +4 \ MATHCAL {K} _ {11}^2 $。
The information of the event-by-event fluctuations is extracted from flow harmonic distributions and cumulants, which can be done experimentally. In this work, we employ the standard method of Gram-Charlier series with the normal kernel to find such distribution, which is the generalization of recently introduced flow distributions for the studies of the event-by-event fluctuations. Also, we introduce a new set of cumulants $j_n\{2k\}$ which have more information about the fluctuations compared with other known cumulants. The experimental data imply that not only all of the information about the event-by-event fluctuations of collision zone properties and different stages of the heavy-ion process are not encoded in the radial flow distribution $p(v_n)$, but also the observables describing harmonic flows can generally be given by the joint distribution $\mathcal{P}(v_1,v_2,...)$. In such a way, we first introduce a set of joint cumulants $\mathcal{K}_{nm}$, and then we find the flow joint distribution using these joint cumulants. Finally, we show that the Symmetric Cumulants $SC(2,3)$ and $SC(2,4)$ obtained from ALICE data are explained by the combinations $\mathcal{K}_{22}+\frac{1}{2}\mathcal{K}_{04}-\mathcal{K}_{31}$ and $\mathcal{K}_{22}+4\mathcal{K}_{11}^2$.