Fig. 1. Schematic phase diagram of QCD matter in temperature-baryon chemical potential-rotation axes^[6]

Fig. 2. Phase diagram of the T-Ω plane^[6]

Fig. 3. Phase diagram of the ω-µI plane for QCD^[28]

Fig. 4. Phase diagrams of (T, Ω) plane at the chiral MIT boundary condition for cylinder with radius R = 20/Λ^[23]

Fig. 5. Radial dependence of chiral condensate for different rotations of ω=0.5[exp(1.5r-r02)+1]-1 (a) andω=0.06[expr-10+1]-1 (b)^[27]

Fig. 6. The dynamical mass as a function of Ω andeB corresponding to strong coupling (a) and weak coupling (b)^[34]

Fig. 7. Diagram showing energy-level splitting under the combined influence of external magnetic and vortex fields^[25]

Fig. 8. Under the contribution of gluon polarization, the chiral phase transition temperature as a function of the angular velocity^[82]

Fig. 9. Phase diagrams of T-ω plane for EMD model^[83] (a) and two-flavor AdS/QCD model^[31] (b)

Fig. 10. Global polarization difference between Λ and its antiparticle under different magnetic field lifetimes as a function of collision energy^[58] (a), comparison between the AMPT model simulation and the STAR experiment of global polarization^[53] (b)

Fig. 11. Rapidity-azimuth distribution of the local spin polarization of Λ andΛ¯ for Au+Au collisions at 20%~50% centrality range at 19.6 GeV and 200 GeV, respectively^[59]

Fig. 12. Local polarizations as functions of azimuthal angles for different definitions of vorticity^[83]