Journal of the American Chemical Society
COMMUNICATION
Figure 1. Solid-state structures for (a) (tbsL)Fe3(thf) (1), (b) [(tbsL)Fe3(μ3-N)][NBu4] (2) (side view in d), and (c) (tbsL)Fe3(μ3-NMe) (3) (side
view in e) with the thermal ellipsoids set at the 50% probability level (hydrogen atoms, solvent molecules, and Bu4N cation in 2 omitted for clarity; Fe
orange, C black, H white, N blue, O red, Si pink). Bond lengths (Å) for 1: Fe1-Fe2, 2.6129(5); Fe1-Fe3, 2.5061(5); Fe2-Fe3, 2.6118(5); Fe-Nbase
,
2.047(2); Fe-Ntbs, 1.950(2); Fe-O, 2.1162(18); for 2: Fe1-Fe2, 2.4212(7); Fe1-Fe3, 2.5444(7); Fe2-Fe3, 2.4737(7); Fe-N7avg, 1.871(3); Fe-
N
base, 2.030(3); Fe-Ntbs, 1.950(3); for 3: Fe1-Fe2, 2.449(3); Fe1-Fe3, 2.487(2); Fe2-Fe3, 2.513(2); Fe-N7avg, 1.892(3); N7-C43, 1.457(14);
Fe-Nbase, 1.996(10); Fe-Ntbs, 1.904(10).
overall yield (80%, Scheme 1). Crystallographic analysis of single
crystals of 1 provided the composition consisting of three iron
ions and an asymmetrically bound hexaamide ligand (Figure 1a).
Unlike the trinuclear complexes we have previously reported, the
large silyl substituents on the ligand platform prevent two of the
three apical amide groups from bridging adjacent metal ions.
Only a single silylamide bridges Fe1 and Fe2, while the other two
silylamides are terminally bound to Fe2 and Fe3, giving each iron
ion a distinct coordination environment. The average Fe-Fe
separation is 2.577(6) Å, which is comparable to that for
previously reported complexes.4 The zero-field 57Fe M€ossbauer
spectrum of 1 reflects its asymmetry as the 110 K spectrum can
only be modeled using three quadrupole doublets (δ, |ΔEQ|
The ligand reorganization accommodates binding of the monatomic
nitride ligand. The nitride is heavily pyramidalized (Σ(Fe-N7-Fe)
= 248.94(14)°, NH3 is 319.8°), sitting 1.205(3) Å above the triiron
basal plane. The solution magnetic moment for paramagnetic 2 is
7.3(2) μB, while the zero-field 57Fe M€ossbauer spectrum of 2
obtained at 120 K shows two quadrupole doublets (δ, |ΔEQ|
(
mm/s)): component 1 0.37, 1.78 (48%); component 2 0.39, 1.23
(51%)). The lower isomer shift of 2 compared to 1 reflects the
increased oxidation of the trinuclear core.4
In contrast to the electrophilic nature of terminal Fe-nitride
complexes,6 the nucleophilicity of the nitride in complex 2 can be
demonstrated by its rapid reaction with methyl iodide to afford a
hexane-soluble methyl imido complex (tbsL)Fe3(μ3-NCH3) (3)
with generation of Bu4NI. Previous examples of triiron imido
complexes were synthesized via reaction of iron carbonyl pre-
cursors with silylazide, nitroarene, or alkyldiazene reagents.10
Storing complex 3 in hexanes at -33 °C deposited crystals
suitable for X-ray diffraction analysis. The solid-state molecular
structure for 3 is shown in Figure 1c. Structurally similar to 2,
complex 3 features a central μ3-imide ligand with average Fe-N
and Fe-Fe bond lengths of 1.892(3) and 2.483(3) Å, respec-
tively. The imide ligand sits 1.265(9) Å above the triiron basal
plane, slightly extended from the nitride (see core highlights
shown in Figure 1d and e). Like 2, the zero field 57Fe M€ossbauer
spectrum of paramagnetic 3 (5.3(2) μB) obtained at 110 K shows
two quadrupole doublets with identical isomer shifts (δ, |ΔEQ|
(
mm/s)): component 1 0.89, 1.68; component 2 0.49, 1.57; com-
ponent 3 0.50, 1.92). The 1H NMR silent material is consistent
with the large solution magnetic moment for paramagnetic 1
(12.0(2) μB) determined by the Evans’ method.
Reaction of complex 1 with tetrabutylammonium azide at
room temperature results in the dissociation of thf from 1 and
consumption of the azide as judged by the absence of the azide
stretch (νN3) in the IR spectrum. Storing the reaction product in
diethyl ether at -33 °C deposited crystals of the reaction product
suitable for X-ray diffraction analysis. The solid-state molecular
structure for the product, shown in Figure 1b, confirmed the
breakdown of the azide to produce the nearly C3-symmetric
nitride product [(tbsL)Fe3(μ3-N)]NBu4 (2) (Scheme 1).
While formation of iron-nitride complexes proceeding via
thermal or photolytic decomposition of iron azides embedded in
tetraazamacrocylic ligand environments is well precedented,7
most polynuclear (nuclearity exceeding two) iron-nitride spe-
cies form via reduction of nitrosyl ligands8 or via metathetical
routes using N(SnMe3)3.9 However, these routes give rise to
unpredictable nuclearity and cluster geometries. Formation of
the anionic nitride 2 proceeds via the two-electron oxidation of 1
where the overall complex geometry is dictated by the trinucleat-
ing ligand (tbsL).
(
mm/s)): component 1 0.36, 1.67 (65%); component 2 0.37, 0.94
(35%)). Obtaining a spectrum at 180 K causes the two quadru-
pole doublets to coalesce (δ, |ΔEQ| (mm/s)): 0.34, 1.44), sug-
gesting the Fe nuclei relax faster than the M€ossbauer time scale
(10-7 s).
In summary, the silyl-substituted ligand platform [tbsL]6-
supports triiron complex formation, maintaining a degree of
coordinative unsaturation at the iron ions. Despite the asymme-
try of the triiron thf-bound complex, the compound rapidly reacts
with a single equivalent of inorganic azide to produce a nearly C3-
symmetric, μ3-nitride complex. The observed nucleophilic re-
activity of the anionic nitride demonstrates the utility of embed-
ding a polynuclear reaction site within a single ligand manifold.
This strategy permits control of the nuclearity of the resultant
complex and elaboration of a cooperatively bound substrate, as
demonstrated by alkylation of the nitride to afford a bridging
Complex 2 features three iron centers that bind the central μ3-
nitride ligand with average Fe-N and Fe-Fe bond lengths of 1.871
(3) and 2.480(1) Å, respectively. Each of the iron ions sit in dis-
torted tetrahedral, nearly cis-divacant octahedral, sites, bridged by two
ligand internal amide residues (average Fe-Nbase 2.030(3) Å) and
capped by one terminal silyl-amide (average Fe-Ntbs 1.950(3) Å).
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dx.doi.org/10.1021/ja2003445 |J. Am. Chem. Soc. 2011, 133, 3336–3338