We study the locked-unlocked transition for a class of lasers with inj
ected signal. The transition is produced by a parametric breaking of t
he invariant circle that represents the free running laser. A Hopf-sad
dle-node codimension two bifurcation coupled with a phase-drift re-inj
ection mechanism organizes the flow. Fixed points (locked states), per
iodic orbits and tori, T-2, of two inequivalent types as well as heter
o-homoclinic loops are found by using methods of bifurcation theory an
d are illustrated with computer simulations. We discuss the dependence
of the flow patterns with respect to the laser parameters and, in par
ticular, we show that the detuning between atomic and cavity frequenci
es plays a fundamental role for the dynamics.