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Figure 1.The lattice QCD result of the Dirac eigenvalue distributionphase ( ρ(λ) in thelattice unit for (a) the confinement phase (β = 5.6, 103 ×5) and (b) the deconfinementβ = 6.0, 103 × 5)
Figure 2.(a) A simple example of the temporally odd-number lattice (Nt = 3 case).(b) Only gauge-invariant quantities such as closed loops and the Polyakov loop survivein QCD
Table 1.Numerical lattice-QCD results for LHS (of the relation (16) in the confinement phase withIR Dirac-mode cutoff of ΛLP ) and RHS (Dirac spectral sum) β = 5.6 on 103 × 5 size lattice foreach gauge configuration (labeled with “Config
Figure 4.(a) The scatter plot of the Polyakov loop in lattice QCD. The originalfigure is taken from Ref.[33].(b) The temperature dependence of the Polyakovloop susceptibilities ratio RA ≡ χA/χL and the light-quark chiral condensate ⟨ψψ ¯⟩l,normalized to its
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