  We study the profile of the broken string (flux tube) in the maximally
abelian gauge below and above the finite temperature phase transition in full
QCD. In the deconfinement phase, the flux tube disappears and the electric
field apperas to be Coulomb-like. In the confinement phase, but near $T_c$, at
shorter distances a flux tube is formed like at zero temperature, while at
larger distances the tube disappears similar to the deconfinement phase.
