Angewandte
Chemie
evidenced by its solid-state magnetic moment of about
2.21 mB, and accordingly has one unpaired electron. The
electronic absorption spectrum of 2 displays a strong absorp-
tion at 250 nm arising from the ligands and two absorptions at
389 and 572 nm with e = 2055 and 2730 molÀ1 LcmÀ1.
is perpendicular to the z axis, which is clearly consistent with
the anisotropic EPRspectra of 2. Fivefold bonding between
two Cr atoms, arising from a s2p4d3 configuration for the Cr2
core is consequently implied. The bonding scheme of 2 was
further corroborated by unrestricted DFT calculations
(BP86), and the metal–metal orbital surfaces are shown in
Figure S2 (Supporting Information). The symmetries of
SOMO and SOMOÀ1, mainly dx2Ày2 + dx2Ày2 and dxy + dxy,
correspond to d bonds. The SOMOÀ2, dz2 + dz2, corresponds
to Cr–Cr s bonding, while SOMOÀ3 and SOMOÀ5, dxz + dxz
The solid-state molecular structure of compound 2
(Figure 1) was deciphered by X-ray crystallography.[19] In
À
and dyz + dyz, are Cr Cr p bonds. The nondegeneracy of
SOMO and SOMOÀ1 is consistent with the Jahn–Teller
structural distortion observed in complex 2.[23]
The cyclic voltammogram of a solution of 2 (THF/
tetrabutylammonium phosphate) shows a reversible reduc-
tion wave at E1/2 = À2.14 V (relative to Fc/Fc+) over the
course of the cathodic sweep. Accordingly, reduction of THF
solutions of 2 with KC8 in the presence of 4,7,13,16,21,24-
hexaoxa-1,10-diazabicyclo[8.8.8]hexacosane
(crypt[222])
gave extremely air- and moisture-sensitive dark purple
species K(crypt[222])[Cr2{ArXylNC(H)NArXyl}3] (K(crypt-
[222])[3]) in 83% yield. After workup the product showed a
diamagnetic NMRspectrum in [D 8]THF with sharp resonan-
1
ces between d = 0 and 8 ppm for H, and d = 0 and 230 ppm
for 13C. The electronic absorption spectrum of 3 has a strong
absorption at 250 nm and a broad absorption at 488 nm, with
e = 3200 molÀ1 LcmÀ1.
The solid-state molecular structure of 3 (Figure 2) was
elucidated by X-ray crystallography.[19] In comparison with
the distorted structure of 2, the lantern structure is still
conserved, except that it displays a more symmetrical D3-
symmetric structure (Figure 2b). The most remarkable fea-
ture of 3 is that the Cr–Cr bond contracts significantly to a
distance of 1.7397(9) , a difference of about 0.08 when
compared to 2. The FSRof the Cr–Cr bond in 3 is 0.733. The
magnitude of this change suggests that the additional electron
resides in the dx2Ày2- or dxy-based molecular orbital if the z axis
is coincident with the Cr–Cr bond, and therefore the dimetal
core has a s2p4d4 configuration. The increase in average Cr–N
distance from 2.044(3) in 2 to 2.092(3) in 3 on one-electron
reduction indicates substantially weaker interactions between
Cr and ligands compared to quadruply bonded
Figure 1. Solid-state structure of [Cr2(ArXylNC(H)NArXyl)3] (2) viewed
a) normal to and b) along the metal–metal axis with thermal ellipsoids
at 30% probability.
contrast to the D3h-symmetric trigonal paddlewheel Fe and
Co amidinates,[20,21] in which all degenerate molecular orbitals
are evenly occupied, 2 is substantially distorted from D3
symmetry (Figure 1b), as evidenced by significant deviation
from trigonal geometry at both Cr atoms with N-Cr1-N bond
angles of 106.96(10), 123.15(11), and 125.53(11)8, and N-Cr2-
N
bond angles of 107.57(10), 126.00(10), 122.73(11)8.
Cr2(amidinate)4 complexes,[4] which, as
a consequence,
Although contributions from packing forces can not be
completely ignored,[20] the structural distortion of 2 is
essentially attributed to the Jahn–Teller effect[22] (vide
infra). The metal–metal bond length of 1.8169(7) for 2 is
significantly shorter than the Cr–Cr quintuple-bond length of
1.8351(4) of complex [Ar’CrCrAr’].[12] Complex 2 has a
formal shortness ratio (FSR) of 0.766 (cf. FSR(N2) = 0.786).[4]
Since 2 has one unpaired electron, we subjected it to a
detailed EPRstudy. In toluene 2 is EPR-silent at room
temperature, but axial symmetry displayed at low temper-
ature (77 K) suggests that the unpaired electron resides in an
orbital perpendicular to the z axis (coincident with the Cr–Cr
axis), namely, dx2Ày2 or dxy (Figure S2, Supporting Informa-
tion). In fact, DFT calculations on complex 2 reproduced the
geometrical features of the solid-state structure of 2. The
calculated SOMO has mostly metal dx2Ày2 character and hence
enhance the overlap of dx2Ày2 and dx2Ày2, and dxy and dxy, to
form two d bonds. The extremely short Cr–Cr bond of 3 is the
shortest known metal–metal bond in an isolable compound. It
is also the first metal–metal bond shorter than 1.8 , and it
lies in the range of those of hypothetical quintuply bonded
Cr–Cr complexes.[11]
We examined the nature of the bonding in 3 by DFT
calculations (BP86). The geometry of the optimized structure
was in close agreement with the crystal structure of 3.
Considerable metal–metal bonding can be found from
HOMO to HOMOÀ4 (Figure 3). Orbital HOMOÀ2 corre-
sponds the Cr–Cr s bond (dz2 + dz2), while the degenerate
HOMOÀ3 and HOMOÀ4 display Cr–Cr p-bonding inter-
actions (dxz + dxz and dyz + dyz). Almost degenerate Cr–Cr d-
bonding character is apparently displayed by HOMO (dx2Ày2
+
d
x2Ày2) and HOMOÀ1 (dxy+dxy). In contrast to the significant
Angew. Chem. Int. Ed. 2008, 47, 7250 –7253
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7251