  We consider a linear chain made of spins of one half in contact with a
dissipative environment for which periodic delta-kicks are applied to the
qubits of the linear chain in two different configurations: kicks applied to a
single qubit and simultaneous kicks applied to two qubits of the linear chain.
In both cases the system reaches a non-equilibrium stationary condition in the
long time limit. We study the transient to the quasi stationary states and
their properties as function of the kick parameters in the single kicked qubit
case and report the emergence of stationary entanglement between the kicked
qubits when simultaneous kicks are applied. For doing our study we have derived
an approximation to a master equation which serves us to analyze the effects of
a finite temperature and the zero temperature environment.
