Trigonal Mn3 and Co3 Clusters
Supported by Weak-Field Ligands: A Structural, Spectroscopic, Magnetic,
and Computational Investigation into the Correlation of Molecular
and Electronic Structure
posted on 2016-02-20, 10:20authored byAlison
R. Fout, Dianne J. Xiao, Qinliang Zhao, T. David Harris, Evan R. King, Emily V. Eames, Shao-Liang Zheng, Theodore A. Betley
Transamination of divalent transition metal starting
materials
(M2(N(SiMe3)2)4, M = Mn,
Co) with hexadentate ligand platforms RLH6 (RLH6 = MeC(CH2NPh-o-NR)3 where R = H, Ph, Mes (Mes = Mesityl)) or H,CyLH6 = 1,3,5-C6H9(NHPh-o-NH2)3 with added pyridine or tertiary phosphine
coligands afforded trinuclear complexes of the type (RL)Mn3(py)3 and (RL)Co3(PMe2R′)3 (R′ = Me, Ph). While the sterically
less encumbered ligand varieties, HL or PhL,
give rise to local square-pyramidal geometries at each of the bound
metal atoms, with four anilides forming an equatorial plane and an
exogenous pyridine or phosphine in the apical site, the mesityl-substituted
ligand (MesL) engenders local tetrahedral coordination.
Both the neutral Mn3 and Co3 clusters feature S = 1/2 ground states, as determined
by direct current (dc) magnetometry, 1H NMR spectroscopy,
and low-temperature electron paramagnetic resonance (EPR) spectroscopy.
Within the Mn3 clusters, the long internuclear Mn–Mn
separations suggest minimal direct metal–metal orbital overlap.
Accordingly, fits to variable-temperature magnetic susceptibility
data reveal the presence of weak antiferromagnetic superexchange interactions
through the bridging anilide ligands with exchange couplings ranging
from J = −16.8 to −42 cm–1. Conversely, the short Co–Co interatomic distances suggest
a significant degree of direct metal–metal orbital overlap,
akin to the related Fe3 clusters. With the Co3 series, the S = 1/2 ground
state can be attributed to population of a single molecular orbital
manifold that arises from mixing of the metal- and o-phenylenediamide (OPDA) ligand-based frontier orbitals. Chemical
oxidation of the neutral Co3 clusters affords diamagnetic
cationic clusters of the type [(RL)Co3(PMe2R)3]+. Density functional theory (DFT)
calculations on the neutral (S = 1/2) and cationic (S = 0) Co3 clusters
reveal that oxidation occurs at an orbital with contributions from
both the Co3 core and OPDA subunits. The predicted bond elongations
within the ligand OPDA units are corroborated by the ligand bond perturbations
observed by X-ray crystallography.