  We present here a formalism able to generalise to a relativistically
covariant scheme the standard nuclear shell model. We show that, using some
generalised nuclear Green's functions and their Lehmann representation we can
define the relativistic equivalent of the non relativistic single particle wave
function (not loosing, however, the physical contribution of other degrees of
freedom, like mesons and antinucleons). It is shown that the mass operator
associated to the nuclear Green's function can be approximated with the
equivalent of a shell-model potential and that the corresponding ``single
particle wave functions'' can be easily derived in a specified frame of
reference and then boosted to any other system, thus fully restoring the
Lorentz covariance
