  We investigate the deconfining phase transition in full QCD with two flavors
of staggered fermions in presence of a constant abelian chromomagnetic field.
We find that the deconfinement temperature decreases and eventually goes to
zero by increasing the strength of the chromomagnetic field. Moreover our
results suggest that the chiral transition coincides with the deconfinement
transition and therefore even the chiral critical temperature depends on the
applied chromomagnetic field. We also find that the chiral condensate increases
with the strength of the chromomagnetic field.
