• NUCLEAR TECHNIQUES
  • Vol. 46, Issue 4, 040002 (2023)
Shi YIN, Yangyang TAN, and Weijie FU*
Author Affiliations
  • School of Physics, Dalian University of Technology, Dalian 116024, China
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    DOI: 10.11889/j.0253-3219.2023.hjs.46.040002 Cite this Article
    Shi YIN, Yangyang TAN, Weijie FU. Critical phenomena and functional renormalization group[J]. NUCLEAR TECHNIQUES, 2023, 46(4): 040002 Copy Citation Text show less
    Schematic phase diagram of QCD
    Fig. 1. Schematic phase diagram of QCD
    Flow diagram of RG equations around the Gaussian fixed point in dimensions (a) d>4, (b)2<d<4
    Fig. 2. Flow diagram of RG equations around the Gaussian fixed point in dimensions (a) d>4, (b)2<d<4
    (a) Flow diagram of RG equations around the W-F fixed point in 2<d<4, (b) critical exponentν in the order ofO(ε) at the W-F fixed point obtained in the plane ofN of theO(N) symmetry and the dimensiond
    Fig. 3. (a) Flow diagram of RG equations around the W-F fixed point in 2<d<4, (b) critical exponentν in the order ofO(ε) at the W-F fixed point obtained in the plane ofN of theO(N) symmetry and the dimensiond
    Critical exponent ν in the limit of largeN→∞ as a function of the spatial dimensiond calculated with different values of the expansition orderntrunc
    Fig. 4. Critical exponent ν in the limit of largeN as a function of the spatial dimensiond calculated with different values of the expansition orderntrunc
    2D plot of the critical exponent ν as functions of the spatial dimensiond and the symmetryN calculated with different values of the expansition orderntrunc
    Fig. 5. 2D plot of the critical exponent ν as functions of the spatial dimensiond and the symmetryN calculated with different values of the expansition orderntrunc
    Exact results of the critical exponent ν as functions of the spatial dimensiond and the symmetryN with the truncation LPA
    Fig. 6. Exact results of the critical exponent ν as functions of the spatial dimensiond and the symmetryN with the truncation LPA
    R42B=χ4B/χ2B,R62B=χ6B/χ2B andR82B=χ8B/χ2B as functions of the temperature at vanishing baryon chemical potential (μB=0) in comparison with lattice results[92]
    Fig. 7. R42B=χ4B/χ2B,R62B=χ6B/χ2B andR82B=χ8B/χ2B as functions of the temperature at vanishing baryon chemical potential (μB=0) in comparison with lattice results[92]
    R42B,R62B andR82B as functions of the temperature with different values ofμB in the range of0~400 MeV[92]
    Fig. 8. R42B,R62B andR82B as functions of the temperature with different values ofμB in the range of0~400 MeV[92]
    Chemical freeze-out temperature and baryon chemical potential in the T-μB plane. The blue pentagons and red circles show the freeze-out data from Andronic et al and STAR experiment, respectively[92]
    Fig. 9. Chemical freeze-out temperature and baryon chemical potential in the T-μB plane. The blue pentagons and red circles show the freeze-out data from Andronic et al and STAR experiment, respectively[92]
    Baryon number fluctuations R42B in theT-μB plane as well as the freeze-out curve: STAR Fit II[92]
    Fig. 10. Baryon number fluctuations R42B in theT-μB plane as well as the freeze-out curve: STAR Fit II[92]
    Baryon number fluctuations R42B,R62B andR82B as functions of the collision energy obtained in QCD-assisted LEFT in comparison to the STAR data[92]
    Fig. 11. Baryon number fluctuations R42B,R62B andR82B as functions of the collision energy obtained in QCD-assisted LEFT in comparison to the STAR data[92]
    Shi YIN, Yangyang TAN, Weijie FU. Critical phenomena and functional renormalization group[J]. NUCLEAR TECHNIQUES, 2023, 46(4): 040002
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