The continuous parametric pumping of a superconducting lossy QED cavity sup
porting a field prepared initially as a superposition of coherent states is
discussed. In contrast to classical pumping, we verify that the phase sens
itivity of the parametric pumping makes the asymptotic behaviour of the cav
ity field state strongly dependent on the phase theta of the coherent state
\ alpha > = \ alpha \e(i theta)>. Here we consider theta = pi /4, -pi /4 a
nd we analyse the evolution of the purity of the superposition states with
the help of the linear entropy and fidelity functions. We also analyse the
decoherence process quantitatively through the Wigner function, for both st
ates, verifying that the decay is slightly modified when compared to the fr
ee decoherence case: for theta = -pi /4 the process is accelerated while fo
r theta = pi /4 it is delayed.