Chemical oxidation and reduction
of the all-ferrous (HL)2Fe6 in THF
affords isostructural, coordinatively
unsaturated clusters of the type [(HL)2Fe6]
n
: [(HL)2Fe6][BArF24] (1, n = +1; where [BArF24]− = tetrakis[(3,5-trifluoromethyl)phenyl]borate),
[Bu4N][(HL)2Fe6] (2a, n = −1), [P][(HL)2Fe6] (2b, n = −1;
where [P]+ = tributyl(1,3-dioxolan-2-ylmethyl)phosphonium),
and [Bu4N]2[(HL)2Fe6] (3, n = −2). Each member
of the redox-transfer series was characterized by zero-field 57Fe Mössbauer spectroscopy, near-infrared spectroscopy,
single-crystal X-ray crystallography, and magnetometry. Redox-directed
trends are observed when comparing the structural metrics within the
[Fe6] core. The metal octahedron [Fe6] decreases
marginally in volume as the molecular reduction state increases as
gauged by the Fe–Feavg distance varying from 2.608(11)
Å (n = +1) to 2.573(3) (n =
−2). In contrast, the mean Fe–N distances and ∠Fe–N–Fe
angles correlate linearly with the [Fe6] oxidation level,
or alternatively, the changes observed within the local Fe–N4 coordination planes vary linearly with the aggregate spin
ground state. In general, as the spin ground state (S) increases, the Fe–N(H)avg distances also increase.
The structural metric perturbations within the [Fe6] core
and measured spin ground states were rationalized extending the previously
proposed molecular orbital diagram derived for (HL)2Fe6. Chemical reduction of the (HL)2Fe6 cluster results in an abrupt increase in spin
ground state from S = 6 for the all-ferrous cluster,
to S = 19/2 in the monoanionic 2b and S = 11 for the dianionic 3. The observation of asymmetric intervalence charge transfer bands
in 3 provides further evidence of the fully delocalized
ground state observed by 57Fe Mössbauer spectroscopy
for all species examined (1–3). For
each of the clusters examined within the electron-transfer series,
the observed spin ground states thermally persist to 300 K. In particular,
the S = 11 in dianionic 3 and S = 19/2 in the monoanionic 2b represent the highest spin ground states isolated up to
room temperature known to date. The increase in spin ground state
results from population of the antibonding orbital band comprised
of the Fe–N σ* interactions. As such, the thermally persistent
ground states arise from population of the resultant single spin manifolds
in accordance with Hund’s rules. The large spin ground states,
indicative of strong ferromagnetic electronic alignment of the valence
electrons, result from strong direct exchange electronic coupling
mediated by Fe–Fe orbital overlap within the [Fe6] cores, equivalent to a strong double exchange magnetic coupling B for 3 that was calculated to be 309 cm–1.