Angewandte
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Figure S4; Table S3) with a four-coordinate planar
geometry at both the copper and the nickel centers,
and geometrical parameters in excellent agreement
with that obtained from XAS studies (Table S2). In the
calculated structure MeAN acts as a bidentate ligand,
with one of the terminal tertiary amine nitrogen atoms
remaining out of the coordination sphere of Cu. The
ground state is calculated to be S = 1/2, consistent with
the EPR studies. The unpaired spin is distributed such
that the nickel center has 0.7 spin, whilst the copper and
oxygen centers carry an average spin density of only
0.01 and 0.06, respectively (Table S4). These results
reveal the presence of NiIII (S = 1/2; 3d7) and CuIII (S =
0; 3d8) centers in 3, thereby, supporting a [LNiIII(m-
O)2CuIII(MeAN)]+ assignment. Vibrational analysis on
the DFT-optimized structure of 3 in the S = 1/2 ground
state predicts a strong [NiIII(m-O)2CuIII]2+ core vibra-
tional mode at 640 cmÀ1 (Figures S5–S6; Table S5). This
frequency and in particular the calculated 18O/16O
isotopic shifts are in excellent agreement with the
experimental data (Figure 1). Thus, the spectroscopic
results validate the calculated molecular and electronic
structures of 3.
Figure 2. A) Normalized Cu K-edge XANES spectra for 2-BF4 (dotted line),
3 (dash–dot line), and 4 (solid line). The inset depicts an expansion of the pre-
edge region for 3 and 4. B) Normalized Ni K-edge XANES spectra for 1 (solid
line) and 3 (dash–dot line). The inset shows an expansion of the pre-edge
region. C) Fourier-transformed Cu K-edge EXAFS spectra of 2-BF4 and 3
(Experiment: dotted line; simulation: bold line). D) Fourier-transformed Ni K-
edge EXAFS spectra of 1 and 3. For the EXAFS data on a wavevector scale
before calculation of the Fourier transform see Figure S3.
The oxo groups in high-valent [M2(m-O)2]n+ (M =
Fe, Co, Ni, Cu) cores act as strong electrophiles and are
typically unreactive towards other electrophiles.[2] Con-
sistent with these observations, addition of cyclohexane
carboxaldehyde (CCA) or 2-phenylpropionaldehyde (2-
PPA) to [(AN)2Cu2(m-O)2]2+ [5,14] or [(L)2Ni2(m-O)2],[15] which
are the homometallic analogues of 3, at À908C does not
change the UV/Vis spectra. In contrast, similar reactions with
3 result in instantaneous bleaching and disappearance of the
bands at 370 and 895 nm in the UV/Vis absorption spectrum
(Figure S7). Product analysis of the reaction mixture reveals
the formation of the deformylated[16] products in 65–90%
yields (Scheme 1; Table S6). The reactivity of 3 was further
investigated using benzoyl chloride at À508C, to confirm the
nucleophilic properties of 3. A pseudo-first order decay of the
absorption feature at 895 nm and the subsequent formation of
benzoic acid (Figure S8) were observed upon adding benzoyl
chloride to a preformed solution of 3 at À508C. The rate
constant increases proportionally with the substrate concen-
tration, affording a second-order rate constant, k2, of
0.11mÀ1 sÀ1 at À508C. Additional mechanistic studies with
para-substituted benzoyl chloride (para-Y-C7H4OCl; Y=
OMe, Me, H, Cl, CN) reveal a good linear correlation of
the rate to the sP+ values of the para substituents. A positive
Hammett 1 value of 2.5 (Figure S9) is obtained, which further
supports the nucleophilic character of the [LNiIII(m-O)2CuIII-
(MeAN)]+ core in the oxidation of benzoyl chloride. To our
knowledge, 3 is the only example of a high-valent[6] bis(m-oxo)
dimetal complex containing nucleophilic oxo groups. To
investigate in how far the dangling amine group assists
reactivity or is even responsible for the observed nucleophi-
licity, experiments with N,N,N’,N’-tetramethylethylenedia-
mine (TMEDA), as a co-ligand for Cu instead of MeAN
were envisaged. Unfortunately, unlike 2-BF4, the CuI-
(TMEDA) complex has been reported to be unstable,[17] so
that it had to be generated in situ prior to the reaction with 1.
3.[12] The X-band EPR spectrum (Figure 1) of 3 is also found
to be in good agreement with the [LNiIII(m-O)2CuIII(MeAN)]+
assignment and is dominated by a typical S = 1/2 NiIII rhombic
signal (gx = 2.006, gy = 2.14, gz = 2.41) that lacks the hyperfine
splitting characteristic of CuII,[13] and corresponds, by inte-
gration, to 90% of the amount of 2-BF4 added. The absence of
hyperfine splitting indicates copper in the diamagnetic 3d8
low-spin state, which moreover reveals planar coordination.
Extended X-ray absorption fine structure (EXAFS)
analysis reveals further structural details (Figure 2C; Fig-
ure 2D and S3; Table S1). For 1 a shell of four N/O scatterers
at 1.84 ꢀ is obtained from Ni EXAFS, in good agreement
with the molecular structure determined previously by X-ray
crystallography (Table S2).[4] On the other hand, a fit to the
data for 3 requires two subshells of N/O scatterers at 1.79 ꢀ
(assigned to the two NiIII O units) and 1.88 ꢀ (assigned to the
À
two NiIII N units), consistent with the structure derived from
À
DFT calculations (Table S2). In addition, Ni EXAFS of 3
shows an additional peak at 2.81 ꢀ corresponding to the Cu
scatterer, thereby strongly supporting the presence of a het-
erodinuclear Ni···Cu center in 3. Further support for including
a Ni···Cu distance at 2.81 ꢀ comes from Cu EXAFS, which
also detects the Ni scatterer at 2.81 ꢀ in 3, but not in the
mononuclear CuI precursor. Furthermore, the best fit of the
Cu EXAFS of 3 can be obtained with two subshells, each
containing two O/N scatterers at 1.80 ꢀ and 2.00 ꢀ, thereby
supporting a four coordinate Cu center in 3. It is important to
note that a fit with two O/N scatterers at 1.88 ꢀ and three O/
N scatterers at 2.00 ꢀ gave a high Debye–Waller factor, which
together with the DFT calculations (see below) preclude the
presence of a five-coordinate Cu center in 3 (Table S1).
DFT calculations (see Supporting Information for details)
on 3 yield a minimum energy for a C1 structure (Scheme 1;
Angew. Chem. Int. Ed. 2013, 52, 1 – 6
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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