2 research outputs found
High Spin Co(I): High-Frequency and -Field EPR Spectroscopy of CoX(PPh<sub>3</sub>)<sub>3</sub> (X = Cl, Br)
The previously reported pseudotetrahedral Co(I) complexes,
CoX(PR<sub>3</sub>)<sub>3</sub>, where R = Me, Ph, and chelating analogues,
and X = Cl, Br, I exhibit a spin triplet ground state, which is uncommon
for Co(I), although expected for this geometry. Described here are
studies using electronic absorption and high-frequency and -field
electron paramagnetic resonance (HFEPR) spectroscopy on two members
of this class of complexes: CoX(PR<sub>3</sub>)<sub>3</sub>, where
R = Ph and X = Cl and Br. In both cases, well-defined spectra corresponding
to axial spin triplets were observed, with signals assignable to three
distinct triplet species, and with perfectly axial zero-field splitting
(zfs) given by the parameter <i>D</i> = +4.46, +5.52, +8.04
cm<sup>–1</sup>, respectively, for CoCl(PPh<sub>3</sub>)<sub>3</sub>. The crystal structure reported for CoCl(PPh<sub>3</sub>)<sub>3</sub> shows crystallographic 3-fold symmetry, but with three structurally
distinct molecules per unit cell. Both of these facts thus correlate
with the HFEPR data. The investigated complexes, along with a number
of structurally characterized Co(I) trisphosphine analogues, were
analyzed by quantum chemistry calculations (both density functional
theory (DFT) and unrestricted Hartree–Fock (UHF) methods).
These methods, along with ligand-field theory (LFT) analysis of CoCl(PPh<sub>3</sub>)<sub>3</sub>, give reasonable agreement with the salient
features of the electronic structure of these complexes. A spin triplet
ground state is strongly favored over a singlet state and a positive,
axial <i>D</i> value is predicted, in agreement with experiment.
Quantitative agreement between theory and experiment is less than
ideal with LFT overestimating the zfs, while DFT underestimates these
effects. Despite these shortcomings, this study demonstrates the ability
of advanced paramagnetic resonance techniques, in combination with
other experimental techniques, and with theory, to shed light on the
electronic structure of an unusual transition metal ion, paramagnetic
Co(I)
Low-Spin Hexacoordinate Mn(III): Synthesis and Spectroscopic Investigation of Homoleptic Tris(pyrazolyl)borate and Tris(carbene)borate Complexes
Three complexes of Mn(III) with “scorpionate”
type ligands have been investigated by a variety of physical techniques.
The complexes are [Tp<sub>2</sub>Mn]SbF<sub>6</sub> (<b>1</b>), [Tp<sub>2</sub>*Mn]SbF<sub>6</sub> (<b>2</b>), and
[{PhB(MeIm)<sub>3</sub>}<sub>2</sub>Mn](CF<sub>3</sub>SO<sub>3</sub>) (<b>3a</b>), where Tp<sup>–</sup> =
hydrotris(pyrazolyl)borate anion, Tp*<sup>–</sup> = hydrotris(3,5-dimethylpyrazolyl)borate
anion, and PhB(MeIm)<sub>3</sub><sup>–</sup> = phenyltris(3-methylimidazol-2-yl)borate
anion. The crystal structure of <b>3a</b> is reported; the structures
of <b>1</b> and <b>2</b> have been previously reported,
but were reconfirmed in this work. The synthesis and characterization
of [{PhB(MeIm)<sub>3</sub>}<sub>2</sub>Mn]Cl (<b>3b</b>) are also described. These complexes are of interest in
that, in contrast to many hexacoordinate (pseudo-octahedral) complexes
of Mn(III), they exhibit a low-spin (triplet) ground state, rather
than the high-spin (quintet) ground state. Solid-state electronic
absorption spectroscopy, SQUID magnetometry, and high-frequency and
-field electron paramagnetic resonance (HFEPR) spectroscopy were applied.
HFEPR, in particular, was useful in characterizing the <i>S</i> = 1 spin Hamiltonian parameters for complex <b>1</b>, <i>D</i> = +19.97(1), <i>E</i> = 0.42(2) cm<sup>–1</sup>, and for <b>2</b>, <i>D</i> = +15.89(2), <i>E</i> = 0.04(1) cm<sup>–1</sup>. In addition, frequency
domain Fourier-transform THz-EPR spectroscopy, using coherent synchrotron
radiation, was applied to <b>1</b> only and gave results in
good agreement with HFEPR. Variable-temperature dc magnetic susceptibility
measurements of <b>1</b> and <b>2</b> were also in good
agreement with the HFEPR results. This magnitude of zero-field splitting
(zfs) is over 4 times larger than that in comparable hexacoordinate
Mn(III) systems with <i>S</i> = 2 ground states. Complexes <b>3a</b> and <b>3b</b> (i.e., regardless of counteranion)
have a yet much larger magnitude zfs, which may be the result of unquenched
orbital angular momentum so that the spin Hamiltonian model is not
appropriate. The triplet ground state is rationalized in each complex
by ligand-field theory (LFT) and by quantum chemistry theory, both
density functional theory and unrestricted Hartree–Fock methods.
This analysis also shows that spin-crossover behavior is not thermally
accessible for these complexes as solids. The donor properties of
the three different scorpionate ligands were further characterized
using the LFT model that suggests that the tris(carbene)borate is
a strong σ-donor with little or no π-bonding