论文标题
在RHIC \&LHC ENURGIES中PP,PA和AA碰撞中产生的带电颗粒的多样性和伪含量密度分布
Multiplicity and pseudorapidity density distributions of charged particles produced in pp, pA and AA collisions at RHIC \& LHC energies
论文作者
论文摘要
多重性和假性($η$)密度($ dn _ {\ rm ch}/dη$)的带电载体的分布提供了关键信息,以了解高能重型离子碰撞的粒子生产机制和初始条件。但是,检测器约束限制了可以进行带电粒子测量的$η$范围。通过参数化测得的分布并使用事件发生器的计算来将测得的分布推送到大$η$范围,我们表征了在整个运动学范围内的带电颗粒的产生。在本研究中,我们使用三种不同的Ans $ \ ddot {\ Mathrm a} $ tze来获取对PP,P-A和A-A A-A碰撞碰撞的伪造性HADRON的伪造性分布形状的定量描述($ \ sqrt {$ \ sqrt {对应于RHIC和LHC能量。我们研究了这些碰撞中的限制破碎行为,并报告了TEV量表中高能量碰撞中参与者缩放违规的证据。我们还检查了测得的假性分布,以限制描述颗粒产生初始条件的模型。我们预测带电粒子多重性分布在公平和NICA能量上的中心性依赖性,并为提议的He-lHC和FCC能量提供了带电粒子多重性的估计。
Multiplicity and pseudorapidity ($η$) density ($dN_{\rm ch}/dη$) distributions of charged hadrons provide key information towards understanding the particle production mechanisms and initial conditions of high-energy heavy-ion collisions. However, detector constraints limit the $η$-range across which charged particle measurements can be carried out. Extrapolating the measured distributions to large $η$-range by parameterizing measured distributions and by using calculations from event generators, we characterize the production of charged particles over the full kinematic range. In the present study, we use three different ans$\ddot{\mathrm a}$tze to obtain quantitative descriptions of the shape of pseudorapidity distributions of charged hadrons produced in pp, p-A, and A-A collisions for beam energies ($\sqrt{s_{\rm NN}}$) ranging from a few GeV to a few TeV corresponding to RHIC and LHC energies. We study the limiting fragmentation behavior in these collisions and report evidence for participant-scaling violations in high-energy collisions at the TeV scale. We additionally examine measured pseudorapidity distributions to constrain models describing initial conditions of particle production. We predict the centrality dependence of charged particle multiplicity distributions at FAIR and NICA energies and give an estimation of charged particle multiplicity at $η=0$ for the proposed HE-LHC and FCC energies.