Fig. 3.
(a) The IR-cut Dirac spectral density $\rho _{\rm IR}(\lambda)\equiv \rho (\lambda)\theta (|\lambda |-\Lambda _{\mathrm {IR}})$, and (b) the IR-cut Polyakov loop $\langle L_P\rangle _{\mathrm {IR}}$ on the periodic lattice of $6^4$ at $\beta = 5.6$ for the IR-cut of $\Lambda _{\mathrm {IR}} = 0.5a^{-1}$.

(a) The IR-cut Dirac spectral density |$\rho _{\rm IR}(\lambda)\equiv \rho (\lambda)\theta (|\lambda |-\Lambda _{\mathrm {IR}})$|⁠, and (b) the IR-cut Polyakov loop |$\langle L_P\rangle _{\mathrm {IR}}$| on the periodic lattice of |$6^4$| at |$\beta = 5.6$| for the IR-cut of |$\Lambda _{\mathrm {IR}} = 0.5a^{-1}$|⁠.

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