Antiferromagnetic Co–Gd Interactions in a Tetranuclear [CoGd] 2 Complex with Low‐Spin Square‐Planar Co Ions – Role of the Singly Occupied 3d Co Magnetic Orbital

Structural determinations and magnetic properties of a "chiral at metal" complex and its resulting [Cu-Ln]2 compounds

A chiral trianionic ligand possessing one amide, one imine, two phenol functions and one asymmetric carbon atom into its diamino chain reacts with Cu^II ions to yield anionic [LCu]^- units that crystallize in a non-centrosymmetric space group as infinite 1D zig-zag chains in which a transmission of chirality to the Cu^II ion is effective. The distorted square planar environment of the Cu^II ion is large enough to induce the presence of a stereogenic Cu^II centre. Further reaction with Ln^III ions in presence of ancillary ligands does not preserve such an arrangement but yields a tetranuclear complex made of two [LCu-Ln] units in a head-to-tail position. The tetranuclear [LCu-Ln]₂ complexes made with the racemic and chiral LCu units crystallize in different space groups, so that racemization does not occur. The structural determinations confirm that a symmetry centre is present in the two structures, except for the methyl groups linked to the chiral carbon atoms, which appear as disordered in the (S-S) tetranuclear entity. Such an arrangement implies a conformation change of the diamino chain linked to the Cu^II ion in one [LCu-Ln] unit of the (S-S) entity, and cancels any chirality contribution of the Cu^II ions, as in the meso compound. Ferromagnetic Cu-Ln interactions, resulting from an alternate distribution of the Cu^II and Ln^III ions, are the only ones to be active. Eventually the micro-Squid studies confirm that the hysteresis loops of the corresponding racemate and chiral tetranuclear [LCu-Dy]₂ entities are slightly different.

Contribution of 155Gd Mössbauer data to the study of the magnetic interaction in heterodinuclear 3d–Gd (3d = Cu, Ni) coordination complexes

The observed ¹⁵⁵Gd Mössbauer isomer shifts of 3d–Gd complexes give an experimental proof for the participation of 5d Gd orbitals to the magnetic interaction in these 3d–Gd complexes.