Dramatic differences are found between the ambient and 100 K X-ray structures of [L(2)Ni2Br2](ClO4)2 (L(2) = alpha,alpha'-bis{(5,7-dimethyl-1,4,8,11-tetraazacyclotetradeca-6-yl)-o-xylene), in which the bromide-bridged, bimetallic, macrocyclic ligand complexes of nickel(II) are held face-to-face and in which each bimetallic complex has a net triplet spin multiplicity. The ambient structure of this complex consists of very highly ordered, infinite chains of alternating R and S isomers in which the identical Ni(II) coordination spheres are near to the average expected for the high- and low-spin Ni(II) coordination sites, and there is appreciable stereochemical strain in the linkage of the macrocyclic ligands to the phenyl ring. In contrast, every other dinickel complex of the 100 K structure is displaced about 40 pm along the infinite chains to form tetrameric repeat units (pairs of dinickel complexes), in which each dinickel complex has well-defined high-spin and low-spin Ni(II) coordination sites; the high-spin sites are adjacent in the tetramers, and the stereochemical strain in the linkage to the phenyl spacer is relaxed. The molecular magnetic moments and structural contrasts are similar for the 100 K structure and the previously reported ambient structure of [L(2)Ni2Br3](ClO4) complex for which the molecular magnetic moments also correspond to a single triplet state per complex. The halide-bridged, monochloro- and monobromo dinickel complexes also have triplet spin multiplicity, and they crystallize with a coordinated perchlorate completing the axial coordination of the high-spin Ni(II) site, while the other Ni(II) site of these halide-bridged complexes has equatorial Ni-N bond lengths typical of low-spin Ni(II) coordination. The bridging halide is sandwiched between the face-to-face macrocyclic ligand Ni(II) moieties and slightly off the Ni-Ni axis in all of the complexes. The temperature dependence of the magnetic moments of the series of complexes indicates that their singlet-triplet energy gaps are small, with zero point energy differences that are generally less than 10(3) cm(-1). The very weak metal-metal electronic coupling, the triplet state spin multiplicity of each dinickel complex, and the averaged high-spin/low-spin coordination environments of the ambient structure implicate a vibronic mechanism for the electronic configurational exchange in the dibromo and tribromo complexes. The single molecular vibrational mode that correlates with the configurational exchange in these complexes includes the concerted motion of the bridging bromide between the Ni(II) centers. Activation of this vibrational mode is sufficient to effect the configurational exchange. These complexes present especially clear examples of the effects of the coupling of nuclear vibrational motions to the interchange of electronic configuration between two different centers.

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The syntheses and donor-acceptor properties of some novel, halo-bridged dicopper(II) complexes of alpha,alpha'-bis(5,7-dimethyl-1,4,8,11-tetraazacyclotetradecane-6-yl)-o-xylene are reported. These complexes were characterized by their magnetic and electrochemical behavior, X-ray structure analysis, FAB mass spectroscopy, and electronic spectra. The bromo-bridged complex crystallized in the tetragonal system, space group P4(3)2(1)2, with a = 12.6584(5) A, c = 28.6483 (14) A, Z = 4, R = 0.071, and Rw = 0.147. The chloro-bridged complex crystallized in the monoclinic system, space group C2/c, with a = 32.749(2) A, b = 18.8915(9) A, c = 26.022(2) A, beta =114.831 degrees, Z = 12, R = 0.080, and Rw = 0.132. Both molecules have C2 symmetry. The two copper(II) ions are axially bridged by a bromine or a chlorine, and the two macrocycles are bridged by an o-xylene group. Each complex displays a cofacial ring arrangement. The Cu-X distance (where X = Cl, Br) is shorter than the sum of van der Waals radii of Cu and X. The phenyl ring is approximately orthogonal to the Cu-X-Cu axis. The nonhalo-bridged complex has a significant affinity for halides (Kf approximately 10(4) M(-1)). The chloride-bridged complex had barely resolved differential pulse polarographic waves (DeltaE1/2 approximately 28 mV), while the bromide-bridged complex exhibited two CV waves in the 1.0-1.5 V range (DeltaE1/2 = 0.24 V). All the Cu(II)/Cu(I) couples were irreversible with a cathodic peak at about - 0.9 V. The magnetic susceptibility results below 20 K follow Curie-Weiss behavior, indicating that the magnetic interaction between the two Cu centers is weakly antiferromagnetic with J < or = -1 cm(-1) for all three complexes. A bridging-ligand-mediated superexchange model is used to treat the magnetic and electron-transfer coupling in the Cu(II)(X-)Cu(II) complexes. A single set of perturbation theory parameters is consistent with the magnetic and electrochemical observations on the chloride-bridged complex and the magnetic properties of the bromide-bridged complex. The electrochemical behavior of the latter suggests a relatively low-energy, high-spin configuration for the Cu(III)(Br-)Cu(II) complex. The analysis attributes the weak Cu(II)/Cu(II) coupling to the orthogonality of the donor and acceptor orbitals to the bridging axis. It is inferred that bridging halide-mediated metal-metal dsigma/psigma coupling significantly alters the chemical properties of the bimetallic complexes only when the donor and acceptor orbitals are coaxial with the bridging ligand. In such a limit, the coupling takes the form of a three-center bonding contribution.