The single-crystal
X-ray structure of solvent-free (tmtaa)CoII reveals three
different π–π intermacrocyclic
interactions between tmtaa units (tmtaa = dibenzotetramethyltetraaza[14]annulene).
Pairs of inequivalent (tmtaa)CoII units in the unit cell
link into a one-dimensional π–π stacked array in
the solid state. Magnetic susceptibility (χ) studies from 300
to 2 K reveal the effects of intermolecular interactions between (tmtaa)CoII units in the solid state. The effective magnetic moment
per CoII center is constant at 2.83 μB from 300 to 100 K and begins to significantly decrease at lower
temperatures. The magnetic data are fit to a singlet (S = 0) ground state with a triplet (S = 1) excited
state that is 13 cm–1 higher in energy (−2J = 13 cm–1). Toluene solutions of (tmtaa)CoII have 1H nuclear magnetic resonance (NMR) paramagnetic
shifts, a solution-phase magnetic moment μeff (295
K) of 2.1 μB, and toluene glass electron paramagnetic
resonance spectra that are most consistent with a low-spin (S = 1/2) CoII with the
unpaired electron located in the d
yz
orbital.
Pyridine interacts with (tmtaa)CoII to form a five-coordinate
monopyridine complex in which the unpaired electron is in the d
z
2
orbital. The five-coordinate
complex has been structurally characterized by single-crystal X-ray
diffraction, and the equilibrium constant for pyridine binding at
295 K has been evaluated by both electronic and 1H NMR
spectra. Density functional theory computation using the UB3LYP hybrid
functional places the unpaired electron for (tmtaa)CoII in the d
yz
orbital and that for the
monopyridine complex in the d
z
2
orbital, consistent with spectroscopic observations.