Roles of Bridging Ligand Topology and Conformation in Controlling Exchange Interactions between Paramagnetic Molybdenum Fragments in Dinuclear and Trinuclear Compounds

The magnetic properties of two series of dinuclear complexes, and one trinuclear complex, have been examined as a function of the bridging pathway between the metal centers. The first series of dinuclear complexes is [{MoV(O)(Tp*)Cl}2(í-OO)], where “OO” is [1,4-O(C6H4)nO]2- (n ) 1, 1; n ) 2, 3), [4,4¢-O(C6H3-2-Me)2O]2- (4), or [1,3-OC6H4O]2- (2) [Tp* ) tris(3,5-dimethylpyrazolyl)hydroborate]. The second series of dinuclear complexes is [{MoI(NO)(Tp*)Cl}2(í-NN)], where “NN” is 4,4¢-bipyridyl (5), 3,3¢-dimethyl-4,4¢-bipyridine (6), 3,8-phenanthroline (7), or 2,7-diazapyrene (8). The trinuclear complex is [{MoV(O)(Tp*)Cl}3(1,3,5-C6H3O3)] (9), whose crystal structure was determined [9â5CH2Cl2: C56H81B3Cl13Mo3N18O6; monoclinic, P21/n; a ) 13.443, b ) 41.46(2), c ) 14.314(6) Å; â ) 93.21(3)°; V ) 7995(5) Å3; Z ) 4; R1 ) 0.106]. In these complexes, the sign and magnitude of the exchange coupling constant J is clearly related to both the topology and the conformation of the bridging ligand [where J is derived from H ) -J S1âS2 for 1-8 and H ) -J(S1âS2 + S2âS3 + S1âS3) for 9]. The values are as follows: 1, -80 cm-1; 2, +9.8 cm-1; 3, -13.2 cm-1; 4, -2.8 cm-1; 5, -33 cm-1; 6, -3.5 cm-1; 7, -35.6 cm-1; 8, -35.0 cm-1; 9, +14.4 cm-1. In particular the following holds: (1) J is negative (antiferromagnetic exchange) across the para-substituted bridges ligands of 1 and 3-8 but positive (ferromagnetic exchange) across the meta-substituted bridging ligands of 2 and 9. (2) J decreases in magnitude dramatically as the bridging ligand conformation changes from planar to twisted (compare 3 and 4, or 6 and 8). These observations are consistent with a spin-polarization mechanism for the exchange interaction, propagated across the ð-system of the bridging ligand by Via overlap of bridging ligand p(ð) orbitals with the d(ð) magnetic orbitals of the metals. The EPR spectrum of 9 is characteristic of a quartet species and shows weak ¢ms ) 2 and ¢ms ) 3 transitions at one-half and one-third, respectively, of the field strength of the principal ¢ms ) 1 component.