C O M M U N I C A T I O N S
interaction for the silver species especially in view of the fact that, in
NaAr′GeGeAr′, the “Ar′GeGeAr′” unit formally carries the negative
charge.10
F1 are disordered with respect to a crystallographic inversion center,
and each atom was refined at half-occupancy at the two disordered
sites (see Supporting Information). The Ge-Ag distances (avg.
2.5310(11), 2.7415(12) Å) are unequal with the shorter bond distance
to the fluorinated Ge. The Ge-F distance (1.795(5) Å) is close to that
in compounds (e.g., 1.805(17) Å in [{HC-(CMeNAr)2}GeF] (Ar )
2,6-iPr2C6H3)).14 The Ge-Ge distance (2.4861(12) Å) may be
compared with the 2.44 Å of a single Ge-Ge bond.15 4 can be viewed
as an anionic digermyne fluoride adduct that is π-bonded to two Ag+
ions.16 Its formation and possible resonance structures of the
Ar′GeGe(F)Ar′ monoanion are shown in Scheme 2.
To further understand 2, we performed DFT calculations12 for
the model complex cation Ag(MeGeGeMe)+ (3). This was found
to have an energy minimum whose geometrical parameters compare
well with those found in the X-ray structure of 2. The calculated
HOMO-LUMO gap (71.0 kcal/mol) for 3 is close to the energy
difference of 69.4 kcal/mol suggested by the experimental UV/vis
absorption at 412 nm. Natural bond orbital (NBO) calculations
Scheme 2
In summary, it has been shown that digermyne Ar′GeGeAr′ (1)
reacts with Ag+ at low temperature to form the side-on complex 2.
Its geometry, the Ge-Ge bond lengthening, and calculated electron
densities indicate that the digermyne 1 is acting as a π electron
donor. The exploration of its chemistry is in hand.
reveal that 0.43 electrons are donated from the digermyne
MeGeGeMe to Ag+. According to the calculated second-order
perturbation interaction energies, the strongest orbital interaction
(54.0 kcal/mol) in 3 (and thus in 2) is between the π orbital
(HOMO) of the Ge-Ge bond and the empty 5s or 5p orbitals of
the Ag+ cation, shown above as j and k. The back-donation (l)
from the 4dxz orbital of Ag+ into the empty π* orbital (LUMO+1)
of Ge-Ge (l) is relatively weak (5.5 kcal/mol). Complex 2 is best
described as a hybrid of a π-complex m and a σ-metallacyclopro-
pene structure n shown below.
Acknowledgment. We thank the National Science Foundation
(CHE-0948417) for support of this research.
Supporting Information Available: CIF for 2 and 4, experimental
data, and DFT calculations. This material is available free of charge
References
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The green color of solutions of 2·SbF6 becomes brown when
warmed above ca. 0 °C. Brown crystals of compound [Ag2Ar′GeGe-
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(Scheme 1). The reaction of 1 with AgSbF6 at room temperature also
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unclear, but an abstraction of F from SbF6- to form what may be a
stronger Ge-F bond (bond energy: Ge-F 473, Sb-F 405 kJ/mol) is
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Ge atoms in 2 is probably quite high. The unique structure of 4 (Figure
2) features a near-planar AgGeAgGe core. The atoms Ge1, Ge2, and
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Figure 2. Thermal ellipsoid (50%) drawing of 4 (only one of the disordered
core arrangements is illustrated). H atoms and Pri groups are not shown. Selected
bond distances (Å) and angles (deg): Ag1-Ge2 2.5710(11)Å, Ag1-Ge1
2.7650(12), Ag1′-Ge2 2.4908(11), Ag1′-Ge1 2.7182(11), Ge1-Ge2 2.4861(16),
Ge2-F1 1.795(5), Ag1-C11 2.814(4), Ag1-C12 2.562(3), Ag1-C13 2.820(3),
Ag1-C18 2.642(3), Ag1-Ge2-Ge1 66.274(1), Ag1-Ge1-Ge2 58.3(3),
Ge1-Ag1-Ge2 55.4(4), C1-Ge2-Ge1 124.8(1), F1-Ge2-Ge1 130.8(1),
F1-Ge2-Ag1 102.6(1), C1′-Ge1-Ge2 108.5(1).
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