• NUCLEAR TECHNIQUES
  • Vol. 46, Issue 4, 040011 (2023)
Yin JIANG1、2、* and Jinfeng LIAO3
Author Affiliations
  • 1Beihang University, Beijing 100083, China
  • 2Hangzhou Innovation Institute Yuhang, Beihang University, Hangzhou 310023, China
  • 3Physics Department, Indiana University, Bloomington, IN47405, USA
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    DOI: 10.11889/j.0253-3219.2023.hjs.46.040011 Cite this Article
    Yin JIANG, Jinfeng LIAO. Phase transitions of strong interaction matter in vorticity fields[J]. NUCLEAR TECHNIQUES, 2023, 46(4): 040011 Copy Citation Text show less
    Schematic phase diagram of QCD matter in temperature-baryon chemical potential-rotation axes[6]
    Fig. 1. Schematic phase diagram of QCD matter in temperature-baryon chemical potential-rotation axes[6]
    Phase diagram of the T-Ω plane[6]
    Fig. 2. Phase diagram of the T-Ω plane[6]
    Phase diagram of the ω-µI plane for QCD[28]
    Fig. 3. Phase diagram of the ω-µI plane for QCD[28]
    Phase diagrams of (T, Ω) plane at the chiral MIT boundary condition for cylinder with radius R = 20/Λ[23]
    Fig. 4. Phase diagrams of (T, Ω) plane at the chiral MIT boundary condition for cylinder with radius R = 20/Λ[23]
    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. 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]
    The dynamical mass as a function of Ω andeB corresponding to strong coupling (a) and weak coupling (b)[34]
    Fig. 6. The dynamical mass as a function of Ω andeB corresponding to strong coupling (a) and weak coupling (b)[34]
    Diagram showing energy-level splitting under the combined influence of external magnetic and vortex fields[25]
    Fig. 7. Diagram showing energy-level splitting under the combined influence of external magnetic and vortex fields[25]
    Under the contribution of gluon polarization, the chiral phase transition temperature as a function of the angular velocity[82]
    Fig. 8. Under the contribution of gluon polarization, the chiral phase transition temperature as a function of the angular velocity[82]
    Phase diagrams of T-ω plane for EMD model[83] (a) and two-flavor AdS/QCD model[31] (b)
    Fig. 9. Phase diagrams of T-ω plane for EMD model[83] (a) and two-flavor AdS/QCD model[31] (b)
    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. 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)
    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. 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]
    Local polarizations as functions of azimuthal angles for different definitions of vorticity[83]
    Fig. 12. Local polarizations as functions of azimuthal angles for different definitions of vorticity[83]
    Yin JIANG, Jinfeng LIAO. Phase transitions of strong interaction matter in vorticity fields[J]. NUCLEAR TECHNIQUES, 2023, 46(4): 040011
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