2014/10/31 by V. Voronyuk, V. D. Toneev, В.Д. Тонеев +2 · 5 citations
Physics and Astronomy · #Atomic physics #Charged particle #Condensed matter physics #Electric charge #Electric field #Elliptic flow #Hadron #Heavy ion #High-Energy Particle Collisions Research #Ion #Momentum (technical analysis) #Nuclear physics #Particle physics #Particle physics theoretical and experimental studies #Parton #Physics #Pseudorapidity #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #Quark #Quark–gluon plasma #Quasiparticle #Relativistic Heavy Ion Collider #hep-ph #nucl-th
paper · pdf · doi:10.1103/physrevc.90.064903
published as Phys. Rev. C 90, 064903 (2014) · 8 pages, 12 figures
arxiv created 2014/11/19 · openalex publication_date 2014/12/08 · arxiv updated 2014/12/11 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The directed flow of identified hadrons is studied within the parton-hadron-string-dynamics (PHSD) approach for the asymmetric system Cu + Au in noncentral collisions at √sNN=200 GeV. It is emphasized that due to the difference in the number of protons of the colliding nuclei an electric field emerges, which is directed from the heavy to the light nucleus. This strong electric field is only present for about 0.25 fm/c at √sNN=200 GeV and leads to a splitting of the directed flow v1 for particles with the same mass but opposite electric charges in case of an early presence of charged quarks and antiquarks. The microscopic calculations of the directed flow for \ensuremathπ^\ifmmode±\else\textpm\fi,K^\ifmmode±\else\textpm\fi,p, and p are carried out in the PHSD by taking into account the electromagnetic field induced by the spectators as well as its influence on the hadronic and partonic quasiparticle trajectories. It is shown that the splitting of the directed flow as a function of pseudorapidity \ensuremathη and in particular as a function of the transverse momentum pt provides a direct access to the electromagnetic response of the very early (nonequilibrium) phase of relativistic heavy-ion collisions and allows us to shed light on the presence (and number) of electric charges in this phase.