Spin polarized Fe L 3 M 2,3 M 2,3 and L 3 M 2,3 V Auger-electron spectra were measured and calculated using on-resonance excitation energies of linearly polarized photons ͑at the 2p 3/2 threshold͒ as well as in the offresonance region. Both the intensity distribution and the spin polarization in the experimentally obtained Auger spectra are explained by means of the theoretical model taking into account spin-orbit splitting of core levels and exchange interaction of the core states with the polarized valence band. Different contributions to the Auger spin polarization of both CCC ͑Fe L 3 M 2,3 M 2,3 ) and CCV ͑Fe L 3 M 2,3 V) Auger spectra are discussed. Auger electron spin polarization is positive by transitions to the singlet final two-hole states and is increased with increasing core state-valence state exchange interaction, whereas for the triplet final states the opposite behavior is found.