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arXiv 2007.04194hep-phhep-exnucl-exnucl-th
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在大型强子对撞机上用事件形状和终态多重性破译小碰撞系统中的QCD动力学

Deciphering QCD dynamics in small collision systems using event shape and final state multiplicity at the Large Hadron Collider

Suman Deb, Sushanta Tripathy, Golam Sarwar, Raghunath Sahoo, Jan-e Alam

摘要:

在大型强子对撞机的能量与各种重离子的签名高多重pp碰撞保证了更深入地了解潜在的物理和粒子产生机制。利用强子横动量($p_T$)谱的实验数据提取重离子和高多重数pp碰撞系统的热力学性质是一种常见的做法。由于在$\sqrt{s}$ = 13 TeV的pp碰撞中没有与事件拓扑相关的非奇异和奇异强子谱的实验数据,我们只能利用PYTHIA 8模拟数提取类温度参数来研究比热容、共形对称破缺测度(CSBM)和声速对事件形状和多重数的依赖性.观察到的事件的多重性和事件的拓扑结构有明显的依赖性。系统的热力学很大程度上取决于轻粒子,因为它们的丰度相对较大。在这方面,粒子产生的阈值,$\rm N_{ch} \simeq$(10-20)在最终状态的多重性出现在本研究中,证实了一些早期的发现在这个方向。至于丰度相对较小的重强子,在$\langle \rm N_{ch} \rangle \simeq$ 40中观察到类似的阈值,暗示着所有重强子处于平衡状态的热浴的形成。

英文摘要:

The high-multiplicity pp collisions at the Large Hadron Collider energies with various heavy-ion-like signatures have warranted a deeper understanding of the underlying physics and particle production mechanisms. It is a common practice to use experimental data on the hadronic transverse momentum ($p_T$) spectra to extract thermodynamical properties of the system formed in heavy ion and high multiplicity pp collisions. The non-availability of event topology dependent experimental data for pp collisions at $\sqrt{s}$ = 13 TeV on the spectra of non-strange and strange hadrons constrains us to use the PYTHIA8 simulated numbers to extract temperature-like parameters to study the event shape and multiplicity dependence of specific heat capacity, conformal symmetry breaking measure (CSBM) and speed of sound. The observables show a clear dependence on event multiplicity and event topology. Thermodynamics of the system is largely governed by the light particles because of their relatively larger abundances. In this regards, a threshold in the particle production, $\rm N_{ch} \simeq$ (10-20) in the final state multiplicity emerges out from the present study, confirming some of the earlier findings in this direction. As for heavier hadrons with relatively small abundances, a similar threshold is observed for $\langle \rm N_{ch} \rangle \simeq$ 40 hinting towards formation of a thermal bath where all the heavier hadrons are in equilibrium.

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