Deconfinement transition for nonzero baryon density in the field correlator method

Deconfinement phase transition due to the disappearance of confining colorelectric field correlators is described using a nonperturbative equation of state. The resulting transition temperature T (c) (mu) at any chemical potential mu is expressed in terms of the change of the gluon condensate Delta G(2) and absolute value of the Polyakov loop L-fund(T-c ), which is known from the lattice and analytic data, and is in good agreement with the lattice data for Delta G(2) approximate to 0.0035 GeV4; e.g., T-c (0) = 0.27, 0.19, and, 0.17 GeV for n (f) = 0, 2, and 3, respectively.