Paramagnetic Bis(amidinate) Iron(II) Complexes
FULL PAPER
helpful in establishing their structural relationship, which
was especially useful as 1b could not be crystallized. We are
presently studying the Lewis acidities, electrochemistry, and
photochemistry of the new complexes. Preliminary results
suggest that the binding of the two CO molecules to the
(amidinate)2Fe moiety can be readily reversed upon irradi-
ation.
Experimental Section
General: All experiments were performed under a nitrogen atmo-
sphere using standard Schlenk, glove-box, and vacuum line tech-
niques. All manipulations involving compounds 1 were performed
in the absence of light, the samples being protected by enveloping
glassware in a black plastic bag whenever possible. Solvents (pent-
ane, hexane, THF) were distilled from Na/K alloy prior to use.
Deuterated benzene was dried over Na/K alloy and vacuum trans-
Figure 2. Molecular structure of 2b; hydrogen atoms are omitted
for clarity
˚
Table 2. Selected interatomic distances (A) and bond angles (°)
in 2b
ferred before use. The Li salts Li[tBuC(NR)2] (R ϭ Cy, iPr)[9] and
[12]
anhydrous FeCl2
were prepared according to literature proced-
FeϪN(1)
1.986(1)
2.031(1)
1.771(2)
62.53(5)
90.48(6)
99.85(6)
165.01(5)
93.09(7)
N(1)ϪC(1)
1.342(2)
1.324(2)
1.143(2)
104.21(5)
90.65(6)
163.99(6)
90.01(5)
179.1(1)
FeϪN(2)
N(2)ϪC(1)
ures. Ϫ NMR spectra were recorded on Varian VXR-300 or Unity
500 spectrometers. The 1H NMR spectra were referenced to the
resonances of residual protons in the deuterated solvent. Chemical
shifts (δ) are given relative to tetramethylsilane (downfield shifts
are positive). Ϫ IR spectra were recorded on a Mattson 4020 Gal-
axy FT-IR spectrophotometer. Ϫ Elemental analyses were per-
formed at the Microanalytical Department of the University of
Groningen; all data are the average of at least two independent
determinations. Ϫ Magnetic susceptibility measurements on solid
1a were performed on an MPMS-7 Quantum Design instrument
under zero-field cooled conditions (1000 T field, 5Ϫ300 K temper-
ature range). The EMU and temperature data are the average of
three independent determinations; µeff was calculated from the total
spin quantum number S ϭ 1.96 obtained from the CurieϪWeiss
law (C ϭ 2.90, θ ϭ Ϫ1.35 K).
FeϪC(12)
OϪC(12)
N(1)ϪFeϪN(2)s
N(1)ϪFeϪC(12)
N(1)ϪFeϪC(12a)
N(1)ϪFeϪN(1a)
C(12)ϪFeϪC(12a)
N(1)ϪFeϪN(2a)
N(2)ϪFeϪC(12)
N(2)ϪFeϪC(12a)
N(2)ϪFeϪN(2a)
FeϪC(12)ϪO
The structure is shown in Figure 2, while pertinent in-
teratomic distances and angles are listed in Table 2. The
compound crystallizes in the space group C2/c, with a C2
symmetry axis passing through the Fe atom. The amidinate
ligands are again bound in a dihapto fashion with the
FeNCN ring having a planar geometry [the dihedral angle
FeϪN(1)ϪC(1)ϪN(2) is Ϫ4.6(1)°]. The two Fe-amidinate
planes, related by C2 symmetry, are essentially orthogonal
Preparation of [tBuC(NCy)2]2Fe (1a): All manipulations were per-
formed under the exclusion of light (vide supra). To a stirred sus-
˚
[87.49(8)°]. The FeϪN(2) distance is 0.045 A longer than
the FeϪN(1) distance, as a consequence of the trans-posi- pension of FeCl2 (0.653 g, 5.51 mmol) in THF (40 mL), solid Li[t-
BuC(NCy)2] (2.843 g, 10.5 mmol) was added at ambient temper-
ature. After stirring for 2 h, the solvent was removed in vacuo, and
then any residual THF was removed by stirring the mixture with
pentane (20 mL) and subsequently pumping off the volatiles. Ex-
traction of the residue with pentane (30 mL), concentration of the
extract, and cooling it to Ϫ25 °C afforded 1.640 g (2.81 mmol,
54%) of 1a as analytically pure yellow crystals. Ϫ 1H NMR
([D6]benzene, 25 °C): δ ϭ 188 (∆ν1/2 ϭ 280 Hz, 4 H, iPr CH), 11.9
(∆ν1/2 ϭ 40 Hz, 8 H, Cy CH2), 10.7 (∆ν1/2 ϭ 60 Hz, 8 H, Cy CH2),
9.0 (∆ν1/2 ϭ 60 Hz, 18 H, tBu Me), 2.7 (∆ν1/2 ϭ 470 Hz, 8 H, Cy
tion of N(2) in relation to the CO ligand. Compared to
the two known FeII cis-dicarbonyl complexes with bidentate
monoanionic ligands — the phosphanyl-enolate and phos-
phanyl-carboxylate derivatives [Ph2PCHC(Ph)O]2Fe(CO)2
[10]
[11]
and [Ph2PCH2C(O)O]2Fe(CO)2
— complex 2b has a
much more strongly distorted octahedral geometry. This is
due to the very small ‘‘bite angle’’ of the dihapto amidinate
ligand, i.e. N(1)ϪFeϪN(2) is just 64.53(5)°, as compared to
OϪFeϪP angles of 82Ϫ86° in the other two complexes. In
all three complexes, the CϪFeϪC angle is about 93°, and CH2), 1.5 (∆ν1/2 ϭ 73 Hz, 4 H, Cy CH2), 1.1 (∆ν1/2 ϭ 33 Hz, 4 H,
Cy CH2), 0.5 (∆ν1/2 ϭ 785 Hz, 8 H, Cy CH2). Ϫ 13C{1H} NMR
([D6]benzene, 25 °C): δ ϭ 628 (assignment uncertain), 335 (tBu
hence this feature would appear to be quite insensitive to
changes in the ligand. In the IR spectra, the carbonyl vibra-
Me), 304 (Cy β-CH2), 27.9 (Cy δ-CH2), 20.1 (Cy γ-CH2). Ϫ
tions for 2 are found at noticeably lower wavenumbers than
C34H62N4Fe (582.7): calcd. C 70.08, H 10.72, N 9.61, Fe 9.58;
for the phosphanyl-carboxylate and -enolate complexes
found C 69.74, H 10.79, N 9.39, Fe 9.75.
(2048, 1998 cmϪ1 and 2023, 1969 cmϪ1, respectively), indic-
ating that the amidinate ligands are better donors.
In conclusion, we have prepared two paramagnetic 14-
Preparation of [tBuC(NiPr)2]2Fe (1b): Following a similar proced-
ure as described above for 1a, but using Li[tBuC(NiPr)2] (0.934 g,
4.91 mmol) and FeCl2 (0.308 g, 2.43 mmol), 0.26 g (0.61 mmol,
25%) of crude 1b was obtained as a brown-yellow oil upon evapora-
electron bis(amidinate) iron(II) complexes and their dia-
magnetic 18-electron dicarbonyl derivatives. 1H and 13C
NMR spectroscopy of the paramagnetic complexes proved tion of the solvent from the pentane extract. Ϫ 1H NMR ([D6]ben-
Eur. J. Inorg. Chem. 2001, 707Ϫ711
709