  Coincidence scattering of polarized electrons from nuclei with polarization
transfer to outgoing nucleons is studied within the context of relativistic
mean field theory. Effects introduced by the dynamical enhancement of the lower
components of the bound and scattered nucleon wave functions are analyzed for
the polarized response functions and transferred polarization asymmetries.
Results obtained by projecting out the negative-energy components are compared
with the fully-relativistic calculation. The crucial role played by the
relativistic dynamics in some spin-dependent observables is clearly manifested
even for low/medium values of the missing momentum. Kinematical relativistic
effects are also analyzed. A discussion of the factorization approach and the
mechanism for its breakdown is also briefly presented.
