Table 1. Comparison of selected NMR and structural data of 1,2-disilacy-
clobut-2-enes 5a–e (exptl) and 6a–f (calcd).
29Si (Si=C)[c]
d
13C (Si=C)[c]
ꢀ
Si=C [] Si Si [] SSi [8]
d
5a
5b
5c
5d
5e
1.746(2)
2.3154(5) 356.2(1) 75.0
155.2
185.4
159.6
195.6
175.1
171.5
201.9
179.5
224.2
193.6
153.9
–
–
–
–
–
–
98.6
Scheme 2. 5a: R=Tip, R’=Ph; 5b: R=Si(Me)tBu2, R’=Ph; 5c: R=Tip,
R’=SiMe3; 5d: R=SiMetBu2, R’=SiMe3; 5e: R=SiMetBu2, R’=H.
–
–
–
–
–
–
112.5
139.1
112.5
85.5
118.8
124.8
166.0
127.0
99.6
6a[a] 1.762
6b[b] 1.775
6c[a] 1.748
6d[b] 1.760
6e[b] 1.750
6 f[a] 1.738
2.305
2.326
2.314
2.338
2.345
2.318
360.0
360.0
359.9
360.0
360.0
360.0
and were characterized by multinuclear NMR and UV/Vis
spectroscopy. Additionally, the structure of phenyl substitut-
ed derivative 5a in the solid state was confirmed by single
crystal X-ray diffraction (Figure 1).[15]
[a] B3LYP/6-31 g(d,p). [b] B3LYP/6-31 g(d). [c] GIAO/B3LYP/6-311 g-
G
A
scopic features of a hydrogen directly attached to the
carbon atom of the Si=C bond. While a recently reported
1
hydrosilene exhibited a H NMR shift at d 6.06 ppm for the
hydrogen bonded to the silicon atom of the Si=C moiety;[13]
in the case of 5e a signal at much lower field (7.47 ppm) is
observed probably due to the different electronegativities of
silicon and carbon. This resonance can indeed be unambigu-
ously assigned to the hydrogen at the carbon atom of the
ꢀ
Si C double bond on grounds of its triplet splitting due to
coupling with the adjacent protons of the methylene group
(3J=4.8 Hz). This coupling is significantly higher than that
reported for carbon based cyclobutenes (3J=0.9 to
1.4 Hz).[16] Conversely, the 1J coupling constant of the “vinyl-
ic” proton to the Si=C carbon atom is somewhat smaller in
case of 5e (153.4 Hz) than the corresponding value of
parent cyclobutene (168.5 Hz).[16c] This observation can be
rationalized in terms of the larger covalent radii of the sili-
con atoms in the ring as compared to carbon allowing for
larger inner angles at the endocyclic carbon atoms, which by
Figure 1. Structure of 5a in the solid state. All hydrogen atoms and disor-
dered isopropyl groups removed for clarity. Ellipsoids at 30% probabili-
ꢀ
ꢀ
ty. Selected bond lengths [] and angles [8]: Si1 C2 1.7459(15), Si1 Si2
ꢀ
ꢀ
ꢀ
ꢀ
2.3154(5), Si2 C1 1.9191(16), C1 C2 1.536(2), C2 C3 1.457(2), Si1 C16
ꢀ
ꢀ
1.8729(15), Si2 C31 1.9111(15), Si2 C46 1.9056(14); C2-Si1-C16
127.43(7), C2-Si1-Si2 80.74(5), C16-Si1-Si2 148.06(5), C1-Si2-Si1 74.45(5),
C3-C2-C1 121.45(13), C3-C2-Si1 134.99(12), C1-C2-Si1 103.53(10), C2-
C1-Si2 100.43(9).
ꢀ
consequence should raise the s character of the C C bond
in the four-membered ring and hence the spin couplings
through that bond.
As expected, the NMR data of 5a–e suggest a significant
influence of the substituents on the electronic structure of
the Si=C bond. Trisilyl-substituted disilacyclobutenes 5b,d
show strongly deshielded tricoordinate Si and C atoms com-
pared to those of 5a,c with triaryl substitution of the Si2
moiety (Table 1). Within these two subsets the most shielded
double bond silicon atoms are those of 5a and 5b, respec-
tively, with a phenyl group attached to the Si=C carbon
atom, which may be explained in terms of a reduced polari-
ty of the double bond due to p conjugation with the sub-
stituent. A comparison of the longest-wavelength absorption
maxima in the UV/Vis spectra of 5a,b shows that the influ-
ence of the substituents at silicon on the HOMO–LUMO
gap is negligible (lmax, 5a: 385, 5b: 389 nm). Conversely, the
effect of the phenyl substituent at the Si=C carbon atom is
much more pronounced and responsible for a significant
red-shift (lmax, 5d: 330, 5e: 322 nm), which is widely appre-
ciated as evidence for conjugation.
Single crystals suitable for an X-ray diffraction study were
obtained in case of phenyl substituted 5a (Figure 1) con-
firming the constitution of a 1,2-disilacyclobut-2-ene. The
Si1–C2 distance of 1.7459(15) is within the typical range
of Si=C double bonds[2] Even though the four-membered
ring is slightly twisted (Si2-Si1-C2-C1 7.17(9)8; Si2-C1-C2-
Si1 ꢀ8.69(10)8) the Si=C double bond is essentially planar
(sum of angles Si1 356.2(1), C2 360.0(1)8) in sharp contrast
to the strongly pyramidalized Si=C silicon atom of oxygen
containing 4a–c.[9] The p conjugation of the phenyl group of
5a suggested by the spectroscopic data becomes readily ap-
parent from the co-planar arrangement of the phenyl sub-
stituent with the Si2C2 ring (dihedral angle Si1-C2-C3-C4
5.4(2)8) and the relatively short bond to the ipso-carbon
ꢀ
atom (C2 C3 1.457(2) ). The larger covalent radius of sili-
con compared with carbon indeed imposes small inner
angles at Si1 and Si2 and larger ones at C1 and C2 (Si2-Si1-
C2 80.74(5), C1-Si2-Si1 74.45(5), Si1-C2-C1 103.53(10), C2-
It is important to note that the half-parent system 5e
offers the unprecedented possibility to study the spectro-
7120
ꢀ 2008 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2008, 14, 7119 – 7122