  We show that definite polarization observables for the simplest
electroproduction processes, $\ell+N\to \ell+B(1/2^\pm)+M(0^\pm)$,
$B=Y(\Lambda, \Sigma$ or $Y_c$-hyperon, $\Theta^+$-pentaquark) and $M=K$,
$\bar{K}$ or $D$, are sensitive to the relative P-parity $\pi(B)$ of the
NBM-system. The interference of the longitudinal and transversal amplitudes for
the collinear regime of the processes $\gamma^*+N\to B+M $($\gamma^*$ is the
virtual photon) - at any value of momentum transfer squared and excitation
energy of the $BM$-system - generates model independent relations between
analyzing powers (in unpolarized lepton scattering by polarized target), from
one side, and the components of the produced baryon $B$ polarization. It is
important to stress that these relations depend on the above mentioned
P-parity, and constitute a model independent method for the determination of
unknown parities of strange and charm particles.
