Modeling of Local Strong Parity Non-Conservation Effects in Relativistic Heavy-Ion Collisions

IF 0.3 4区 物理与天体物理 Q4 PHYSICS, NUCLEAR
V. N. Kovalenko, V. V. Petrov
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引用次数: 0

Abstract

The violation of spatial parity symmetry (\(P\)) in strong interactions have never been observed experimentally. However a \(P\)-breaking term can be included in the QCD Lagrangian. Hence, the local parity symmetry breaking can occur due to large topological fluctuations at high temperature with dynamic generation of nontrivial topological charge configurations. A necessary condition for observing these effects is a sufficiently large space dimension and a long lifetime of a hot drop of QCD medium, which is available in central nuclear collisions at the LHC. In order to study the effects caused by local \(P\)-breaking in relativistic heavy-ion collisions we integrated them in Monte Carlo generators. Based on the analysis of the Monte Carlo data on the studied observables, taking into account the responses of the detecting systems of the ALICE facility under LHC Run 2 and Run 3 conditions, recommendations will be given on the criteria for selecting events, tracks, and choosing kinematic variables in terms of increasing sensitivity to the effects of local parity non-conservation.

相对论重离子碰撞中局部强奇偶性非守恒效应建模
强相互作用中空间奇偶对称性(\(P\))的违反从未在实验中被观测到。然而,QCD 拉格朗日中可以包含一个(P)破缺项。因此,局部奇偶对称性破缺可能是由于高温下的大拓扑波动与动态生成的非难拓扑电荷构型而发生的。观测这些效应的一个必要条件是足够大的空间维度和热滴 QCD 介质的长寿命,而这在大型强子对撞机的中心核碰撞中是可以实现的。为了研究相对论重离子对撞中局部(P\)破缺引起的效应,我们在蒙特卡洛发生器中对它们进行了整合。根据对所研究观测指标的蒙特卡洛数据的分析,并考虑到在大型强子对撞机运行2和运行3条件下ALICE设施探测系统的响应,将就事件、轨道的选择标准和运动学变量的选择提出建议,以提高对局域奇偶性不守恒效应的敏感性。
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来源期刊
Physics of Atomic Nuclei
Physics of Atomic Nuclei 物理-物理:核物理
CiteScore
0.60
自引率
25.00%
发文量
56
审稿时长
3-6 weeks
期刊介绍: Physics of Atomic Nuclei is a journal that covers experimental and theoretical studies of nuclear physics: nuclear structure, spectra, and properties; radiation, fission, and nuclear reactions induced by photons, leptons, hadrons, and nuclei; fundamental interactions and symmetries; hadrons (with light, strange, charm, and bottom quarks); particle collisions at high and superhigh energies; gauge and unified quantum field theories, quark models, supersymmetry and supergravity, astrophysics and cosmology.
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