Angewandte
Chemie
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a Si H bond in 3 (see the Supporting Information). Strikingly,
the chemical shift of the two-coordinate silicon atom in 3 in
the 29Si NMR spectrum appears at much higher field (d =
ꢀ83.8 ppm in [D8]THF and d = ꢀ80.1 ppm in C6D6) than that
of the acyclic siladicarbene Si(cAAC)2 E (d = 66.7 ppm in
C6D6). The enormous upfield shift observed for 3 is in
accordance with GIAO calculations (d = ꢀ78.7 ppm). We
reasoned that the remarkable shielding of the 29Si nucleus in 3
results from a stronger s-donor but weaker p-acceptor ability
of the two NHC moieties towards silicon and the acute C-Si-C
angle caused by the cyclic structure. To gain insights into the
electronic differences, we carried out additional computa-
tional investigations of the related model compounds 3’ (with
a chelate bis-NHC), 3’’ (with two NHCs), and E’ (bearing two
cAAC ligands). Selected results of the calculations are
Figure 3. Molecular structure of 3. Ellipsoids are set at 50% proba-
bility. H atoms are omitted for clarity. Selected interatomic distances
[ꢂ] and angles [8]: Si1–C1 1.864(1), Si1–C2 1.874(1), C1–N1 1.383(2),
C1–N2 1.382(2), C2–N3 1.374(2), C2–N4 1.377(2); C1-Si1-C2 89.1(1),
Si1-C1-N2 128.9(1), Si1-C1-N1 127.9(1), N1-C1-N2 103.1(1), Si1-C2-N3
128.4(1), Si1-C2-N4 127.8(1), N3-C2-N4 103.7(1).
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summarized in Table 1. Whereas the C-Si C angle of the
cyclic silylone model 3’ is smaller than that of acyclic silylone
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3’’ and E’, the Si C bond length of 3’ is slightly longer than
Table 1: Calculated distances and angles, 29Si chemical shifts, NBO
charges at Si, and the first and second proton affinities (PAs) of model
compounds 3’, 3’’, and E’.[a]
Crystals of 3 in the monoclinic space group C2/c could be
obtained in toluene solutions at ꢀ208C. The X-ray diffraction
analysis (Figure 3) reveals that the Si atom in 3 is two-
coordinate with a C-Si-C angle of 89.1(1)8, which is much
smaller than those in C (136.58),[7] D (125.78),[8] and E
(117.98),[9] but is comparable to those in the germylone
analogue F (86.68)[11] and in its precursor 2 (88.7(2)8).
The six-membered C3N2Si ring is puckered and adopts
a boat conformation. The dihedral angle between the plane
defined by N2, C3, N3 and the plane defined by C1, C2, N3,
N2 is 508 (versus 46.08 in F,[11] and 35.88 in 2), whereas Si1 is
only slightly deviated from the plane defined by C1, C2, N3,
N2 with corresponding dihedral angle of 10.78 (versus 138 in
F,[11] and 8.18 in 2). The sum of angles around C1 (359.968) and
C2 (359.858) indicates almost ideal trigonal-planar coordina-
3’
3’’
E’
C-Si-C [8]
88.2
1.880
94.7
1.877
100.0
1.861
+25.5
+0.315
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Si C [ꢂ]
d(29Si) [ppm]
NBO charge at
Si
ꢀ69.2
ꢀ67.2
+0.191
+0.163
1st PA [kcal
273.8
164.0
283.4
168.3
268.8
155.3
molꢀ1
]
2nd PA [kcal
molꢀ1
]
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tion geometry of two carbene carbon atoms. The Si C bond
distances in 3 (average 1.869 ꢁ) are significantly shorter than
[a] Calculated at B3LYP/6-31G(d) level of theory. GIAO/B3LYP/6-311(d)
[H, C, N]: 6-311G(3d) [Si].
those in 2 (average 1.962 ꢁ), and in A (1.985(4) ꢁ).[4]
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However, they are distinctly longer than Si C double bonds
that of acyclic silylones. The calculated 29Si chemical shifts and
NBO charges at silicon clearly support that the two NHC
ligands in 3’ and 3’’ are much stronger s-donors towards
silicon than the cAAC ligands in E’. In other words, the Si0
atoms in 3’ and 3’’ are more electron-rich, which explains their
larger first and second proton affinities (PA) in comparison to
E’ (Table 1). The presence of electron-rich silicon(0) in 3
could also explain its extreme sensitivity towards air and
moisture, which is in contrast to the behavior of E.
The UV/Vis spectrum of 3 in toluene solutions exhibits
absorption maxima at l = 345 (e = 4.6 ꢂ 103), 415 (e = 3.5 ꢂ
103), and 547 nm (e = 7.5 ꢂ 103), which are comparable to
those observed for the analogous germylone F (l = 286, 420,
564 nm),[11] the bent trisilaallene C (l = 390, 584),[7] bent
digermasilaallene D (l = 272, 383, 432, 488, and 612 nm),[8]
and E (l = 270, 327, 392, 570, 611 nm).[9] TD-DFT calculations
of compound 3 revealed the longest absorption maximum at
l = 544 nm with an oscillator strength of f = 0.0814, which can
be assigned to the electronic HOMO!LUMO transition.
in silaethenes (1.702–1.775 ꢁ).[14] In fact, they are slightly
longer than that in the siladicarbene (cAAC)2Si
E
(1.841(2) ꢁ),[9a] and close to the calculated value for Si-
(NHC)2 (1.869 ꢁ).[6]
Further insights into the electronic structure of 3 stem
from DFT calculations, which have been carried out for the
silylone 3 at the B3LYP/6-31G(d) level. The optimized
geometry of 3 in the singlet ground state closely reproduced
the experimental data. The energetic gap between singlet
ground state and triplet first excited state is 33.0 kcalmolꢀ1
.
Compound 3 exhibits similar features to those of the
germylone analogue F. For example, the HOMO represents
the silicon p-orbital, whereas the HOMOꢀ1 is the silicon s-
lone-pair orbital (Figure 4). The silicon p-bonding orbital
with Si C bonds presents an evidence for the relatively short
Si C bond length in 3 in comparison to precursor 2. This is
supported by the calculated Si C bond lengths (average
1.888 ꢁ) and the relatively large WBI (Wiberg Bond Index)
values of the Si C bonds (average 1.002). The electronic
nature of silylones has been well-described by Frenking and
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Angew. Chem. Int. Ed. 2013, 52, 7147 –7150
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
7149