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Fourier coefficients of noninterdependent collective motions in heavy-ion collisions

Zhiwan Xu1,*, Gang Wang1,†, Aihong Tang2, and Huan Zhong Huang1,3

  • 1Department of Physics and Astronomy, University of California, Los Angeles, California 90095, USA
  • 2Brookhaven National Laboratory, Upton, New York 11973, USA
  • 3Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), and Institute of Modern Physics, Fudan University, Shanghai-200433, People's Republic of China

  • *zhiwanxu@physics.ucla.edu
  • †gwang@physics.ucla.edu

Phys. Rev. C 107, L061902 – Published 23 June, 2023

DOI: https://doi.org/10.1103/PhysRevC.107.L061902

Abstract

We present a scenario in heavy-ion collisions where different modes of collective motions are noninterdependent, driven by factorized actions in the created nuclear medium. Such physics mechanisms could each dominate at a distinct evolution stage, or coexist simultaneously. If the probability of particle emission is modulated by each nondependent collective motion with a single-harmonic Fourier expansion, the particle azimuthal distribution should be the product of all these expansions. Consequently, nonleading cross terms between collectivity modes appear, and their contributions to experimental observables could be significant. In particular, we argue that the chiral magnetic effect (CME) and elliptic flow can develop separately, with their convolution affecting the observable that is sensitive to the shear-induced CME. We will use the event-by-event anomalous-viscous fluid dynamics model to illustrate the effects of this scenario. Besides giving insights into searches for the CME, we also propose feasible experimental tests based on conventional flow harmonics, and demonstrate the emergence of nonleading cross terms with a multiphase transport model.

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