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Deconfinement phase transition due to disappearance of confiningcolorelectric field correlators is described using nonperturbative equation ofstate. The resulting transition temperature $T_c(\mu)$ at any chemicalpotential $\mu$ is expressed in terms of the change of gluonic condensate$\Delta G_2$ and absolute value of Polyakov loop $L_{fund} (T_c)$, known fromlattice and analytic data, and is in good agreement with lattice data for$\Delta G_2 \approx 0.0035 $ GeV$^4$. E.g. $T_c(0) =0.27; 0.19; 0.17$ GeV for$n_f=0,2,3$ respectively.Comment: 8 pages, 1 figure, LaTeX2e; some typos correcte

Deconfinement transition for nonzero baryon density in the field correlator method