论文标题
$ \ sqrt {s _ {\ mathrm {nn}}}} = 5.02 $ TEV
Light (anti)nuclei production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV
论文作者
论文摘要
在$ \ sqrt {s sqrt {s _ {\ mathrm {nn}}} = 5.02 $ tev中,在$ \ sqrt {s _ {s s _ {s _ {s _ {s _ {s _ {s _ {s _ {s s _ {s _ {s _ {s _ {s s _ {s s _ {s sqrt {测量是在使用爱丽丝探测器的碰撞中心性的函数下以中期($ | y | <$ 0.5)进行的。 $ p _ {\ rm t} $ - 积分产量,结合参数以及与质子和抗抗蛋白质的比率与核合成模型进行了比较。这些结果在不同质量碰撞能的不同碰撞系统中的比较揭示了小型系统中核产生的抑制。在统计强调模型框架中,这可以通过一个较小的相关量来解释,该相关量保守了BARYON数,如先前的波动分析所示。但是,需要不同的相关量大小来描述相同数据集中的质子产量。合并模型可以通过以下事实来描述这种抑制,即核的波函数很大,而火球的大小开始变得可比,甚至比在低多重性下的实际核小得多。
The measurement of the production of deuterons, tritons and $^{3}\mathrm{He}$ and their antiparticles in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is presented in this article. The measurements are carried out at midrapidity ($|y| < $ 0.5) as a function of collision centrality using the ALICE detector. The $p_{\rm T}$-integrated yields, the coalescence parameters and the ratios to protons and antiprotons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-of-mass collision energies reveals a suppression of nucleus production in small systems. In the Statistical Hadronisation Model framework, this can be explained by a small correlation volume where the baryon number is conserved, as already shown in previous fluctuation analyses. However, a different size of the correlation volume is required to describe the proton yields in the same data sets. The coalescence model can describe this suppression by the fact that the wave functions of the nuclei are large and the fireball size starts to become comparable and even much smaller than the actual nucleus at low multiplicities.