Oligosilanes with attached silatranyl units were obtained by reactions of potassium oligosilanides with a silatranyl triflate. Interaction between Si and N atoms was observed in the 29Si NMR spectra (upfield-shifted SiO3 resonances) and in the solid-state structures (Si-N distances between 2.29 and 2.16 Å). The Si-N interaction can be "switched off" either by protonation of the nitrogen lone pair or by potassium silanide formation caused by trimethylsilyl group cleavage in the presence of potassium tert-butoxide.
Oligosilanes with attached silatranyl units were obtained by reactions of potassium oligosilanides with a silatranyl triflate. Interaction between Si and N atoms was observed in the 29Si NMR spectra (upfield-shifted SiO3 resonances) and in the solid-state structures (Si-N distances between 2.29 and 2.16 Å). The Si-N interaction can be "switched off" either by protonation of the nitrogen lone pair or by potassium silanide formation caused by trimethylsilyl group cleavage in the presence of potassium tert-butoxide.
Due to the four valence
electrons that group 14 elements possess,
they exhibit a strong prevalence for tetravalent compounds. However,
even for carbon, compounds with both diminished (lower) and higher
coordination sphere are known. As carbon is a rather small atom, hypervalent
coordination states usually lead to steric interactions between substituents.
Therefore, such situations are typically not stable but only represent
intermediates or transition states, such as in SN2 reactions.[1−3]For the heavier elements silicon, germanium, and tin the situation
is somewhat different. While they share the electronicsituation of
carbon, their atomic radii are larger and therefore they can more
easily accommodate additional substituents. Today, numerous stable
penta- and hexacoordinate compounds are known for silicon,[4−8] germanium,[7−9] and tin.[10−12] In particular, the so-called
atrane molecules (silatranes, germatranes, and stannatranes), substances
which feature the heavy group 14 element with a trialkanolamine ligand
N[(CR1R2)O]3ER (E = Si, Ge), have been studied to quite some extent. In
many cases it was found that hypercoordination has a profound influence
on the bond located trans to the nitrogen atom.Interestingly,
a survey of known sila- and germatranes with different
triethanolamine substituents reveals that, despite the large variety
of attached groups R which have been studied, almost no compounds
of atranes with bonds to other heavy group 14 elements exist.[13,14] Only very recently Zaitsev et al. published a first study addressing
compounds where an atrane unit is attached to a heavy group 14 oligomer
unit.[15] In the current account we want
to present our activities concerning the synthesis and chemistry of
silatranyl-substituted oligosilanes.
Results and Discussion
In recent years we have put some effort into the investigation
of conformational properties of oligosilanes.[16−20] In particular, compounds with bulky end groups such
as the tris(trimethylsilyl)silyl unit were found to exhibit a strong
preference for transoid arrangements of chains. This conformation
is of some importance, as it is known to facilitate the delocalization
of σ-bonding electrons.[21] In addition
to conformational properties, also electronic factors such as substituent
electronegativity[22−26] and hypercoordination[27,28] can influence the optical
absorption properties. We therefore were interested in introducing
silyl substituents into oligosilanes, which have a weakened Si–Si
bond.
Synthesis
One issue that has to be dealt with when
hypercoordinate entities are incorporated into oligosilanes is the
choice of which group should be used. We decided that the plain silatraneconsisting of a silicon atom with a triethanolamine ligand would serve
best as a starting point.In principle there are two ways to
prepare a silatranyl-substituted oligosilane. Either the silatranesilicon atom is introduced first and then the triethanolamine unit
is attached or the silatranyl unit is prepared first and is then attached
as a whole to the oligosilane. After some experiments we found both
strategies possible but concentrated on the second one, which proved
to be more general and gave better yields in our hands.For
the attachment of the silatrane unit the obvious way to proceed
seemed to be reaction of a silatrane with a suitable leaving group
with a silanyl anion. While we found that reactions with silatranylchloride 1 are a possible option, it turned out that
the use of the respective triflate 2 gave better yields.
Synthesis of silatranyl triflate 2 was accomplished by
reaction of silatranyl chloride[29]1 with trimethylsilyl triflate (Scheme ).[30]
Scheme 1
Synthetic
Access to Silatranyl Triflate 2
Reaction of silatranyl triflate 2 with tris(trimethylsilyl)silylpotassium[31] gave the expected neopentasilane 3 in an acceptable yield of 51% (Scheme ). In an analogous way also the related compounds 4 and 5 were obtained.
Scheme 2
Formation of Oligosilanylsilatranes
using Salt Elimination Reactions
With the reaction of isotetrasilanides and 2 being
established, the question arose whether2-trisilanides would also
react the same way. During the course of our studies on oligosilanyl
anions, on several occasions the reactivity of 2-trisilanides differed
substantially from that of isotetrasilanides.[32] However, for the case of the reactions with 2, the
use of a series of 2-trisilanides occurred smoothly. Reaction of 2 with methylbis(trimethylsilyl)silyl potassium gave 6 in a respectable yield of 75%, reflecting the better steric
accessibility of the silanide (Scheme ). With sterically more demanding silanidescarrying
ethyl, isopropyl, and phenyl the reactions also proceeded to 7–9; however, these reactions gave less
satisfying yields (Scheme ).Given the access to this series of oligosilanylsilatranes,
we wanted
to find out whether these compounds could be used as building blocks.
Therefore, compound 3 was reacted with potassium tert-butoxide to cleanly obtain compound 10, which is the product of trimethylsilyl abstraction (Scheme ). An analogous reaction was
carried out with compound 5 to give 11.
In every case attack of the butoxide was selective for a trimethylsilyl
group. When the same reaction was attempted with the alkylated oligosilanylsilatranes 6 and 7, again the expected silatranylsilanides 12 and 13 were formed. However, in these cases
the reactions were not as clean and also attack at the silatranyl
unit was observed, yielding the bis(trimethylsilyl)alkylsilyl potassium
species and the silatranyl tert-butyl ether as side
products. For the methylated substrate 6 the ratio between
the silanide 12 and the silatranyl ether was about 2:1,
whereas for the sterically somewhat better shielded ethylated compound 7 the ratio of 13 to the silatranyl ether was
about 8:1. The phenylated compound 9, however, displayed
a clean reaction with potassium tert-butoxide to
selectively afford silanide 14.
Scheme 3
Formation of Silatranyl
Oligosilanides by Trimethylsilyl Abstraction
For a proper comparison of the UV-absorption properties
of oligosilanes
with and without silatranyl units it was desirable to obtain derivatives
of 2,2,5,5-tetrakis(trimethylsilyl)decamethylhexasilane.[20] Reaction of the respective silanide (Me3Si)3Si(Me2Si)2Si(K)(SiMe3)2[33,34] with 2 did not proceed
to 16 with a satisfactory yield due to the increased
steric bulk of the anion. However, reaction of the anion 10, which was already substituted with silatranyl, with 1-chloro-3,3-bis(trimethylsilyl)heptamethyltetrasilane 15(19) allowed the isolation of compound 16 (Scheme ). Following the same strategy, the 2,5-disilatranylhexasilanecompound 17 was obtained by reaction of 2 equiv of 10 with
1,2-dichlorotetramethyldisilane (Scheme ). Although silanide 10 is sterically
more demanding than tris(trimethylsilyl)silyl potassium it can react
with another equivalent of 2 to give neopentasilane 18 containing two silatranyl units (Scheme ).
Scheme 4
Synthesis of Larger Silatranylated
Oligosilanes 16 and 17
The fact that the silatranenitrogen atom donates
electron density
to the silicon diminishes its basicity. For a number of silatranes,
in particular ones with electronegative substituents, it has been
shown that protonation occurs preferentially at one of the oxygen
atoms, which also exhibit a stronger kinetic basicity.[35,36] Theoretical calculations predict, however, that for a silylated
silatrane protonation should occur preferentially at the nitrogen
atom.[35] To estimate the degree of the nitrogen
donation on the Si–Si bond of 3, it was treated
with trifluoromethanesulfonic acid to protonate the nitrogen lone
pair and thus switch off the Si–N interaction. The obtained
ammonium salt 19·OTf forms cleanly and the shut-off
Si–N interaction is visible in the NMR spectra and the solid-state
structure (Scheme ). While protonation with the extremely strong trifluoromethanesulfonic
acid (pKa = −14)[37] could be expected, an attempt to achieve protonation with
excess acetic acid (pKa = 4.76)[37] failed completely. Reaction of 3 with trichloroacetic acid (pKa = 0.65)[37] was not complete with a stoichiometric amount
of Cl3CCO2H, but a 5-fold excess gave 19·TCA. Other than an osmiumcomplex with a silatranyl
ligand,[38,39]19·OTf seems to be the
only structurally characterized example of a silatrane protonated
at the nitrogen atom.
Scheme 5
Protonation of Silatrane 3 with
Trifluoromethanesulfonic
Acid or Trichloroacetic Acid
NMR Spectroscopy
The compounds of this study were characterized
by multinuclear NMR spectroscopy (Table ). The proton spectra of the neutral compounds
(3–9, 16−18) in CDCl3 exhibit the typical pattern of two
triplets (3JH–H =5.6
Hz) for the two methylene groups of the silatrane unit with chemical
shifts of ca. 3.65 ppm for the O-CH2 units
and 2.72 ppm for the neighboring N-CH2 moieties. It is interesting to note that a relatively strong solvent
effect is observed for the proton spectra, which shall be exemplified
for compound 3, for which the methylene resonances OCH2/CH2N were found at 3.65/2.72 ppm in CDCl3 and 3.30/1.83 ppm in C6D6. The respective 13C resonances of the neutral compounds, which are also all
very similar, were found around 58.5 ppm for the O-CH2 and 51.9 ppm for the N-CH2 units (in both CDCl3 and C6D6).
For the silyl anions 10–14 (in C6D6) the proton resonances shift considerably to
lower field to values around 3.80 ppm for the methylene groups attached
to oxygen atoms and 2.84 ppm for the amino-substituted atoms. The
anioniccompounds exhibit also slightly diminished coupling constants
between the methylene groups. As can be expected, 29Si
NMR spectroscopy provides the most direct insight into the electronicsituation of the compounds involved in this study (Table ).
Table 1
NMR Spectroscopic
Data of Oligosilanyl
Silatranes
29Si
compd
SiMe3
SiO3
Siq
other
13C OCH2/CH2N
1H OCH2/CH2N
3
–9.9
–52.6
–133.9
58.6/52.2a
3.65/2.72a
58.6/51.5b
3.30/1.83b
4
–9.3
–54.0
–132.2
–15.0,
−40.0
58.4/51.9a
3.66/2.73a
5
–9.7
–51.5
–136.8
4.0 (tBuMe2Si)
58.7/52.1a
3.65/2.72a
6
–12.9
–57.8
–88.0
58.3/51.8a
3.69/2.74a
7
–13.2
–56.6
–78.4
58.3/51.9a
3.66/2.71a
8
–13.5
–56.6
–69.6
58.5/52.0a
3.67/2.73a
9
–13.1
–56.6
–76.2
58.1/51.6a
3.75/2.76a
10
–3.2
–11.8
–210.5
61.0./54.3b
3.86/2.84b
11
–3.0
–11.0
–215.7
11.3
61.0/54.2b
3.81/2.82b
12
–5.1
–14.9
–144.0
60.9./54.2b
3.76/2.80b
13
–6.2
–15.0
–125.1
61.0./54.3b
3.88/2.88b
14
–7.7
–19.4
–113.0
61.1/54.2b
3.84/2.81b
16
–9.2/–9.6
–53.8
–128.6/–129.3
–30.6/–30.8 (Me2Si),
58.5/51.8a
3.66/2.73a
17
–9.2
–53.2
–129.5
–31.2
58.8/51.5b
3.36/1.90b
18
–9.5
–46.8
–135.5
59.4/52.7b
3.68/2.71b
19
–9.7
–22.8
–141.1
56.4/53.1b
3.34/2.64b
Measured in CDCl3.
Measured in C6D6.
Measured in CDCl3.Measured in C6D6.To
understand the influence exerted by the nitrogen atom on the
silicon atom in the silatranyl unit, comparison with the chemical
shift of a related trialkoxysilylated oligosilane is required. The
chemical shift of the MeO3Si group of (MeO3Si)4Si[40] is −35 ppm, and thus
the more shielded chemical shift of ca. −53 ppm found for 3–5, 16, and 17 should reflect the degree of hypercoordination (interaction between
Si and N). The respective chemical shifts of compounds 6–9, with more electronegative alkylsilyl substituents,
are further shifted to values close to −57 ppm, thus reflecting
a stronger degree of hypercoordination, which is consistent with what
is observed in the solid-state structures (vide infra). Silatranes,
where the attached silyl group bears only methyl and phenyl groups
such as Me3Si, Me2PhSi, and MePh2Si,[13] which are less electron donating
than the (Me3Si)2SiR groups reported here, allow
an even higher degree of hypercoordination and therefore shift even
further upfield to values of −64.0, −67.0, and −69.0
ppm, respectively.[13] Interestingly, the
chemical shift for the geminal disilatranylsilane 18 of
−46.8 ppm indicates a substantially diminished degree of hypercoordination.
The chemical shift of the respective resonance of 19 at
−22.8 ppm shows the effect of a silatranyl unit with Si–N
interaction turned off by protonation of the nitrogen lone pair. For
the silyl anions 10–14 a downfield
shift of the silatranyl resonance can be expected. Indeed, a shift
from −52.6 ppm for 3 to −11.8 ppm for the
respective anion 10 is observed, which reflects not only
the expected downfield shift of a silyl group in a position α
to a negatively charged atom but also the fact that the Si–N
interaction is turned off in these compounds, as is also clearly visible
in the solid-state structures (vide infra). Another point worth mentioning
is that the 29Si NMR resonances of the negatively charged
silicon atoms in compounds 10 (−210.5 ppm) and 11 (−215.7 ppm) appear at considerably higher field
in comparison to (Me3Si)3SiK (−191.1
ppm).[41] Compounds 11 and 14 are chiral silanides, and 11 is particularly
interesting, as the tert-butyldimethysilyl group
has two diastereotopic methyl groups which allow determination of
the configurational stability of the chiral silanide. Given the additional
coordination to the silatranyl oxygen, an increased configurational
stability might be possible. However, at ambient temperature two different
methyl resonances could not be observed either in the 1H or in the 13C NMR spectrum. Therefore, it has to be
concluded that at room temperature pyramidal inversion of silanide 11 is fast on the NMR time scale.
UV Spectroscopy
The UV absorption spectra of the silatranes 3, 5–9, and 18 exhibit the expected
absorption bands associated with the trisilane
segment around 210 nm only as badly recognizable shoulders. Compound 4, containing a tetrasilane unit, showed an absorption maximum
at 223 nm. For a meaningful comparison to other oligosilanes it is
essential to have compounds with well-resolved absorption bands and
a number of compounds with similar structures. Compounds 16 and 17, with one and two silatranyl units, meet these
requirements and are therefore best suited to estimate the influence
of the siltranyl units on the property of σ-bond electron delocalization.
In order to compare these to structurally related compounds UV spectra
of 2,2,5,5-tetrakis(trimethylsilyl)decamethylhexasilane[42] and 2,5-bis(trimethylsilyl)dodecamethylhexasilane[33] are also shown in Figure .
Figure 1
UV spectra of compounds 16 and 17 and
of [(Me3Si)3SiMe2Si]2 and
[Me(Me3Si)2SiMe2Si]2 in
pentane.
UV spectra of compounds 16 and 17 and
of [(Me3Si)3SiMe2Si]2 and
[Me(Me3Si)2SiMe2Si]2 in
pentane.In the branched oligosilanes with
hexasilane units as the longest
chain segments the effect of the silatranyl units in comparison to
that of trimethylsilyl groups is not very pronounced. For compound 16, containing one silatranyl group, the longest wavelength
absorption band (254 nm) shows a 2 nm hypsochromic shift. The same
band is shifted further toward blue by another 2 nm for compound 17. While the molecular structure of 17 in the
solid state indicates the silatranyl units as part of the all-transoid
hexasilaneconformer, it needs to be pointed out that for 16 and 17 in solution rotation of the bulky tris(silyl)silyl
group is likely to be facile and therefore all-transoid hexasilaneconformers with trimethylsilyl end groups are presumably contributing
to the hexasilane absorption band.Conversely, for 2,5-bis(trimethylsilyl)dodecamethylhexasilane,
where two trimethylsilyl groups are exchanged for methyl groups, the
hexasilane band shows a bathochromic shift of 7 nm to an absorption
maximum of 263 nm. This behavior is consistent with the typically
observed trend of electron-withdrawing substituents causing a bathochromic
shift of the absorption maxima and electron-donating groups being
responsible for contrasting behavior.[43]
Crystal Structure Analysis
Compounds 3, 5–7, 9–11, 14, and 17–19 of this study were subjected to single-crystal XRD analysis. For
compound 3 (Figure ) it was found to be impossible to conduct the measurement
at 100 K, as the crystals at this temperature lost structural integrity.
At 200 K the structure was solved in the triclinic space group P1̅.
Figure 2
Molecular structure of 3 (thermal ellipsoid
plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(1)–O(1)
1.650(3), Si(1)–N(1) 2.292(4), Si(1)–Si(2) 2.3509(18),
Si(2)–Si(3) 2.3351(18), Si(3)–C(13) 1.863(5), N(1)–C(1)
1.462(6), N(1)–C(5) 1.461(5), O(1)–C(2) 1.420(5), C(1)–C(2)
1.522(6); C(1)–N(1)–C(5) 114.4(4), C(2)–O(1)–Si(1)
123.4(3), C(4)–O(2)–Si(1) 123.9(3), C(6)–O(3)–Si(1)
123.6(3).
Molecular structure of 3 (thermal ellipsoid
plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(1)–O(1)
1.650(3), Si(1)–N(1) 2.292(4), Si(1)–Si(2) 2.3509(18),
Si(2)–Si(3) 2.3351(18), Si(3)–C(13) 1.863(5), N(1)–C(1)
1.462(6), N(1)–C(5) 1.461(5), O(1)–C(2) 1.420(5), C(1)–C(2)
1.522(6); C(1)–N(1)–C(5) 114.4(4), C(2)–O(1)–Si(1)
123.4(3), C(4)–O(2)–Si(1) 123.9(3), C(6)–O(3)–Si(1)
123.6(3).Crystals of the more asymmetriccompound 5 (Figure ) were not sensitive
to low temperature and crystallize in the trigonal space group R3̅. Both trimethylsilyl groups and also the tert-butyldimethylsilyl group showed some disorder. The
methylated and ethylated isotetrasilanes 6 (Figure ) and 7 (Figure ) both crystallize
in the orthorhombic space group Pcca, with the latter
compound exhibiting somewhat elongated axes. For 7 some
disorder of the ethyl CH3 group can be found. The phenylated
compound 9 (Figure ) crystallizes in the orthorhombic space group Pca21 with two crystallographically independent
molecules in the asymmetric unit. The silanides 10 (Figure ) and 11 (Figure ) both crystallize
in the monoclinic space group P21/n. For compound 10 some disorder in the silatranyl
unit was found. For the phenylated silanide 14 (Figure ), crystallizing
in the triclinic space group P1̅, an additional
benzene molecule was found in the asymmetric unit. Compound 17 (Figure ) crystallizes in the monoclinic space group P21/c with two crystallographically independent
half-molecules in the asymmetric unit, for which the second halves
are generated by a center of inversion. Also for 17 a
disorderedsilatranyl unit was found. The disilatrane 18 (Figure ) crystallizes
in the monoclinic space group C2/c. The silatranylium triflate 19 (Figure ), which crystallizes in the monoclinic
space group P21/c, shows
three crystallographically independent ion pairs in addition to half
a molecule of benzene on a special position in the asymmetric unit.
The hydrogen attached to the nitrogen atom of 19 was
detected in the experimental electron density map.
Figure 3
Molecular structure of 5 (thermal ellipsoid plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(5)–C(13)
1.883(7), Si(5)–Si(1) 2.3510(18), Si(6)–C(23) 1.885(7),
Si(1)–Si(4) 2.3456(12), Si(1)–Si(2) 2.346(1), Si(2)–O(1)
1.661(2), Si(2)–N(1) 2.283(3), O(1)–C(2) 1.376(4), N(1)–C(1)
1.446(5), C(1)–C(2) 1.393(5); O(3)–Si(2)–O(2)
117.55(15), O(3)–Si(2)–O(1) 116.97(15), O(2)–Si(2)–O(1)
117.83(12), C(5)–N(1)–C(1) 114.4(4).
Figure 4
Molecular structure of 6 (thermal ellipsoid
plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(1)–O(3)
1.670(2), Si(1)–O(1) 1.673(2), Si(1)–O(2) 1.682(2),
Si(1)–N(1) 2.167(3), Si(1)–Si(2) 2.3523(13), Si(2)–C(7)
1.908(3), Si(3)–C(8) 1.871(4), N(1)–C(1) 1.474(4); O(3)–Si(1)–O(1)
117.43(12), O(1)–Si(1)–O(2) 120.09(12), C(1)–N(1)–C(4)
113.7(2).
Figure 5
Molecular structure of 7 (thermal
ellipsoid plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(1)–O(1)
1.671(3), Si(1)–N(1) 2.182(3), Si(1)–Si(2) 2.3443(15),
Si(2)–C(7) 1.907(4), Si(2)–Si(4) 2.3341(17), N(1)–C(2)
1.473(5), O(1)–C(1) 1.409(5); O(1)–Si(1)–O(3)
117.49(14), O(1)–Si(1)–O(2) 120.03(15), O(1)–Si(1)–N(1)
82.58(13), Si(4)–Si(2)–Si(1) 113.38(6), C(6)–N(1)–C(4)
114.1(3).
Figure 6
Molecular structure of 9 (thermal
ellipsoid plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(1)–C(3)
1.910(6), Si(1)–Si(4) 2.342(2), Si(5)–Si(6) 2.383(2),
Si(5)–C(9) 1.904(6), Si(6)–O(4) 1.662(5), Si(6)–O(6)
1.674(5), Si(6)–O(5) 1.682(5), Si(6)–N(2) 2.176(6),
N(1)–C(26) 1.496(8), N(2)–C(32) 1.486(8), O(1)–C(25)
1.430(8); O(4)–Si(6)–O(6) 119.7(3), O(4)–Si(6)–O(5)
118.4(3), O(6)–Si(6)–O(5) 117.3(3), C(36)–N(2)–C(32)
114.2(5).
Figure 7
Molecular structure of 10 (thermal
ellipsoid plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
O(7)–Si(1) 1.659(4), O(7)–K(1) 3.197(5), O(8)–C(15)
1.407(7), O(8)–Si(1) 1.684(4), Si(1)–Si(2) 2.3080(18),
Si(2)–K(1) 3.3634(16), N(1)–C(16) 1.430(7); Si(1)–O(7)–K(1)
97.9(2), C(14)–N(1)–C(16) 119.9(6), C(14)–N(1)–C(17)
122.1(6), C(16)–N(1)–C(17) 117.4(5).
Figure 8
Molecular structure of 11 (thermal ellipsoid
plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–Si(4) 2.2947(12), Si(1)–Si(2) 2.3276(13), Si(1)–Si(3)
2.3391(14), Si(1)–K(1) 3.6321(13), Si(2)–C(19) 1.878(4),
Si(4)–O(8) 1.656(2), Si(4)–K(1) 3.8618(15), O(5)–C(8)
1.430(3), N(1)–C(18) 1.430(4); O(8)–Si(4)–O(9)
105.61(12), O(8)–Si(4)–O(7) 106.14(12), Si(1)–K(1)–Si(4)
35.49(2), C(18)–N(1)–C(14) 119.8(3).
Figure 9
Molecular structure of 14 (thermal ellipsoid
plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–C(22) 1.9141(17), Si(1)–Si(3) 2.3087(7), Si(1)–K(1)
3.5722(9), Si(3)–O(9) 1.6642(12), Si(4)–C(19) 1.8841(19),
K(1)–O(7) 2.9983(12), N(1)–C(16) 1.441(2), O(1)–C(1)
1.421(2); O(9)–Si(3)–K(1) 145.02(5), C(16)–N(1)–C(18)
120.35(14), C(16)–N(1)–C(13) 119.81(14), C(18)–N(1)–C(13)
119.59(14), Si(3)–O(7)–K(1) 111.86(5).
Figure 10
Molecular structure of 17 (thermal ellipsoid
plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–Si(2) 2.3504(18), Si(2)–O(1) 1.657(4), Si(2)–N(1)
2.223(4), Si(3)–C(9) 1.872(7); O(2)–Si(2)–O(3)
117.5(2), N(1)–Si(2)–Si(1) 177.79(14), C(4)–N(1)–C(2)
115.2(6).
Figure 11
Molecular structure of 18 (thermal ellipsoid plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–Si(3) 2.3343(5), Si(1)–Si(2) 2.3416(5), Si(2)–O(2)
1.6512(10), Si(3)–C(9) 1.8728(15), N(1)–C(6) 1.4574(17),
O(1)–C(1) 1.4232(17); Si(3)–Si(1)–Si(2) 108.594(17),
O(2)–Si(2)–O(3) 116.47(5), C(6)–N(1)–C(2)
115.79(12), C(6)–N(1)–C(4) 115.73(11), C(2)–N(1)–C(4)
116.37(11).
Figure 12
Molecular structure
of 19 (thermal ellipsoid plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–Si(5) 2.3072(12), Si(1)–Si(3) 2.3439(13), Si(2)–C(26)
1.868(4), Si(5)–O(11) 1.637(2), N(1)–C(18) 1.503(4),
O(9)–S(3) 1.447(2), O(10)–C(13) 1.414(4), S(3)–C(12)
1.824(4), F(8)–C(12) 1.338(4); Si(5)–Si(1)–Si(3)
105.74(5), Si(5)–Si(1)–Si(4) 107.83(5), O(11)–Si(5)–O(10)
106.94(12), C(18)–N(1)–C(16) 116.8(3).
Molecular structure of 5 (thermal ellipsoid plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(5)–C(13)
1.883(7), Si(5)–Si(1) 2.3510(18), Si(6)–C(23) 1.885(7),
Si(1)–Si(4) 2.3456(12), Si(1)–Si(2) 2.346(1), Si(2)–O(1)
1.661(2), Si(2)–N(1) 2.283(3), O(1)–C(2) 1.376(4), N(1)–C(1)
1.446(5), C(1)–C(2) 1.393(5); O(3)–Si(2)–O(2)
117.55(15), O(3)–Si(2)–O(1) 116.97(15), O(2)–Si(2)–O(1)
117.83(12), C(5)–N(1)–C(1) 114.4(4).Molecular structure of 6 (thermal ellipsoid
plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(1)–O(3)
1.670(2), Si(1)–O(1) 1.673(2), Si(1)–O(2) 1.682(2),
Si(1)–N(1) 2.167(3), Si(1)–Si(2) 2.3523(13), Si(2)–C(7)
1.908(3), Si(3)–C(8) 1.871(4), N(1)–C(1) 1.474(4); O(3)–Si(1)–O(1)
117.43(12), O(1)–Si(1)–O(2) 120.09(12), C(1)–N(1)–C(4)
113.7(2).Molecular structure of 7 (thermal
ellipsoid plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(1)–O(1)
1.671(3), Si(1)–N(1) 2.182(3), Si(1)–Si(2) 2.3443(15),
Si(2)–C(7) 1.907(4), Si(2)–Si(4) 2.3341(17), N(1)–C(2)
1.473(5), O(1)–C(1) 1.409(5); O(1)–Si(1)–O(3)
117.49(14), O(1)–Si(1)–O(2) 120.03(15), O(1)–Si(1)–N(1)
82.58(13), Si(4)–Si(2)–Si(1) 113.38(6), C(6)–N(1)–C(4)
114.1(3).Molecular structure of 9 (thermal
ellipsoid plot drawn
at the 30% probability level). All hydrogen atoms are omitted for
clarity. Selected bond lengths (in Å) and angles (in deg): Si(1)–C(3)
1.910(6), Si(1)–Si(4) 2.342(2), Si(5)–Si(6) 2.383(2),
Si(5)–C(9) 1.904(6), Si(6)–O(4) 1.662(5), Si(6)–O(6)
1.674(5), Si(6)–O(5) 1.682(5), Si(6)–N(2) 2.176(6),
N(1)–C(26) 1.496(8), N(2)–C(32) 1.486(8), O(1)–C(25)
1.430(8); O(4)–Si(6)–O(6) 119.7(3), O(4)–Si(6)–O(5)
118.4(3), O(6)–Si(6)–O(5) 117.3(3), C(36)–N(2)–C(32)
114.2(5).Molecular structure of 10 (thermal
ellipsoid plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
O(7)–Si(1) 1.659(4), O(7)–K(1) 3.197(5), O(8)–C(15)
1.407(7), O(8)–Si(1) 1.684(4), Si(1)–Si(2) 2.3080(18),
Si(2)–K(1) 3.3634(16), N(1)–C(16) 1.430(7); Si(1)–O(7)–K(1)
97.9(2), C(14)–N(1)–C(16) 119.9(6), C(14)–N(1)–C(17)
122.1(6), C(16)–N(1)–C(17) 117.4(5).Molecular structure of 11 (thermal ellipsoid
plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–Si(4) 2.2947(12), Si(1)–Si(2) 2.3276(13), Si(1)–Si(3)
2.3391(14), Si(1)–K(1) 3.6321(13), Si(2)–C(19) 1.878(4),
Si(4)–O(8) 1.656(2), Si(4)–K(1) 3.8618(15), O(5)–C(8)
1.430(3), N(1)–C(18) 1.430(4); O(8)–Si(4)–O(9)
105.61(12), O(8)–Si(4)–O(7) 106.14(12), Si(1)–K(1)–Si(4)
35.49(2), C(18)–N(1)–C(14) 119.8(3).Molecular structure of 14 (thermal ellipsoid
plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–C(22) 1.9141(17), Si(1)–Si(3) 2.3087(7), Si(1)–K(1)
3.5722(9), Si(3)–O(9) 1.6642(12), Si(4)–C(19) 1.8841(19),
K(1)–O(7) 2.9983(12), N(1)–C(16) 1.441(2), O(1)–C(1)
1.421(2); O(9)–Si(3)–K(1) 145.02(5), C(16)–N(1)–C(18)
120.35(14), C(16)–N(1)–C(13) 119.81(14), C(18)–N(1)–C(13)
119.59(14), Si(3)–O(7)–K(1) 111.86(5).Molecular structure of 17 (thermal ellipsoid
plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–Si(2) 2.3504(18), Si(2)–O(1) 1.657(4), Si(2)–N(1)
2.223(4), Si(3)–C(9) 1.872(7); O(2)–Si(2)–O(3)
117.5(2), N(1)–Si(2)–Si(1) 177.79(14), C(4)–N(1)–C(2)
115.2(6).Molecular structure of 18 (thermal ellipsoid plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–Si(3) 2.3343(5), Si(1)–Si(2) 2.3416(5), Si(2)–O(2)
1.6512(10), Si(3)–C(9) 1.8728(15), N(1)–C(6) 1.4574(17),
O(1)–C(1) 1.4232(17); Si(3)–Si(1)–Si(2) 108.594(17),
O(2)–Si(2)–O(3) 116.47(5), C(6)–N(1)–C(2)
115.79(12), C(6)–N(1)–C(4) 115.73(11), C(2)–N(1)–C(4)
116.37(11).Molecular structure
of 19 (thermal ellipsoid plot
drawn at the 30% probability level). All hydrogen atoms are omitted
for clarity. Selected bond lengths (in Å) and angles (in deg):
Si(1)–Si(5) 2.3072(12), Si(1)–Si(3) 2.3439(13), Si(2)–C(26)
1.868(4), Si(5)–O(11) 1.637(2), N(1)–C(18) 1.503(4),
O(9)–S(3) 1.447(2), O(10)–C(13) 1.414(4), S(3)–C(12)
1.824(4), F(8)–C(12) 1.338(4); Si(5)–Si(1)–Si(3)
105.74(5), Si(5)–Si(1)–Si(4) 107.83(5), O(11)–Si(5)–O(10)
106.94(12), C(18)–N(1)–C(16) 116.8(3).The number of structures determined in the course
of this study
allows a fair assessment of the influence of the silatranyl unit on
the oligosilane structure. The most important structural values with
respect to this are the Si–N distance and the bond between
the silatranyl unit and the oligosilane (Table ).
Table 2
Compilation of Structural
Data Derived
by Single-Crystal XRD Analysis of 3, 5–7, 9–11, 14,
and 17–19
compd
dSi··N (Å)
dSi–SiO3 (Å)
dSi–SiMe3 (Å)
dSi–R (Å)
∠Me3SiSiR (deg)
3
2.292(3)
2.351(2)
2.335(2)–2.341(2)
5
2.283(2)
2.346(1)
2.341(1)–2.346(1)
2.351(3)
6
2.167(3)
2.352(1)
2.339(1)/2.346(1)
1.908(3)
7
2.182(4)
2.344(2)
2.334(2)/2.356(2)
1.907(5)
9
2.162(5)
2.383(2)
2.342(2)–2.358(2)
1.904(6)/1.911(7)
10
3.134(4)
2.308(2)
2.312(2)/2.318(2)
3.363(2)
103.42(7)
11
3.184(3)
2.295(1)
2.328(1)
2.339(1)/3.632(1)
104.65(5)
14
3.103(2)
2.3088(8)
2.3431(8)
1.914(2)/3.5722(8)
100.25(5)
17
2.223(4)/2.209(4)
2.350(2)/2.342(2)
2.343(2)–2.346(2)
2.358(2)-2.369(2)
18
2.421(1)
2.3415(5)
2.3343(5)
19
3.394(3)/3.389(3)/3.397(3)
2.301(1)/2.304(1)/2.307(1)
2.339(1)–2.351(1)
For the chlorosilatrane 1 the Si–N distance
has been determined to be 2.023 Å.[5] For the isotetrasilanyl-substituted compounds 3 (Figure ) and 5 (Figure ) elongated
distances of 2.293(3) and 2.283(2) Å consistent with the more
electron donating and sterically much more demanding character of
the attached silyl substituents were found. For compounds 6 (Figure ), 7 (Figure ), and 9 (Figure ) the smaller size of the attached group but also its more
electronegative character of the alkyl and aryl substituents cause
a shortening of the Si–N distances to values of 2.167(3), 2.182(4),
and 2.162(5) Å. The respective value for a PhMe2Si-substituted
silatrane was found to be even shorter: 2.153(2) Å.[13]The Si–SiO3 distances
of 3, 5–7, and 9 are 2.351(2),
2.346(1), 2.352(1), 2.344(2), and 2.383(2) Å, respectively, which
are rather typical Si–Si bond lengths observed in oligosilanes.
Along with the silanide formation, which causes a localization of
negative charge on the silicon atom trans to the nitrogen, an interaction
between silicon and nitrogen is no longer observable in compounds 10, 11, and 14. The Si–N
distances are between 3.10 and 3.18 Å. Along with this shut-off
Si–N interaction Si–SiO3 bond distances of
2.308(2), 2.295(1), and 2.3088(8) Å for 10, 11, and 14 are substantially shorter than those
in the neutral compounds 3, 5, and 9, indicating nondisturbed Si–Si bonds. The structural
motif of the silanides 10, 11, and 14 is different from the usual potassium silanide crown ethercomplexes. Typically the position of the potassium atom in the solid-state
structure is that of a tetrahedral substituent. Complexes 10, 11, and 14 show a distortion of the potassium
position in order to coordinate to one of the silatrane oxygen atoms.
A similar coordination situation was observed for the case of (Me3Si)2Si(K)OMe.[44] This
coordination behavior is taken to an extreme by Krempner’s
silanides (MeOMe2Si)3SiK[45] and (MeOCH2CH2OMe2Si)3SiK,[46] where the potassium ion
only coordinates to the alkoxy groups. However, the Si–K distances
of 10, 11, and 14 are comparable
to what was observed for (Me3Si)3SiK·18-crown-6[41] and also the distances between potassium and
the silatranyl oxygen are only slightly elongated in comparison to
K–O distances of the crown ether. The structural properties
of compound 17 were expected to be close to those of 3 and 5. However, the Si–N distances of
the two crystallographically independent molecules of 17 are 2.223(4) and 2.209(4) Å and thus are significantly shorter,
while the Si–SiO3 bond distances are comparable
to those of 3 and 5. The two independent
molecules exhibit all-transoid hexasilaneconformations, with the
silatranylsilicon atoms being starting and ending points of this
particular conformational subunit.Then again, in accordance
with what was found by NMR spectroscopy
for the geminal disilatrane 18, the respective Si–N
distance for 18 is 2.421(1) Å, being the longest
of the neutral silatranyloligosilanes, but still the Si–SiO3 bond distance is in the same range as for all the other neutral
compounds. For the protonated silatrane 19 no interaction
between silicon and nitrogencan be detected; the Si–N distances
for the three crystallographically independent molecules are around
3.39 Å (Table ), which is even longer than those for the silanidecases of 10, 11, and 14. Accordingly, the
Si–SiO3 bond distances are shortened (2.301(1)/2.304(1)/2.307(1)
Å) to about the same extent that was detected for 10, 11, and 14. The triflatecounterions
are situated above the silatraneclose to the protonated nitrogen
with H–O distances between 1.73(2) and 1.76(2) Å.
Conclusion
Although silatranes are a substance class that has been known for
some time, almost no examples exist with silyl substituents. Our interest
in the chemistry and properties of oligosilanes led us to investigate
possibilities to attach silatranyl units to oligosilanes. While reactions
of potassium oligosilanides with chlorosilatrane did not give the
expected compounds in satisfactory yields, it was found that analogous
reactions with a silatranyl triflate give the oligosilanylated silatranes
in acceptable yields.29Si NMR spectroscopy clearly
suggests a Si–N
interaction, as indicated by upfield-shifted SiO3 resonances.
In addition, the solid-state structures with Si–N distances
between 2.29 and 2.16 Å are supportive of this. Weakening of
the Si–Si bond trans to the Si–N interaction, however,
becomes only obvious upon comparing the Si–Si distances of
structurally related compounds with the Si–N interaction either
active or “turned off” by protonation of the nitrogen
lone pair. Accordingly, the weakening of the (Me3Si)3Si–Si bond by the silatrane effect accounts to an elongation
of about 0.05 Å.Attempts to submit the obtained oligosilanlysilatranes
to further
silanide formation by reaction with potassium tert-butoxide were successful. By single-crystal XRD analysis and multinuclear
NMR spectroscopy it was found that upon silanide formation again the
silatraneSi–N interaction is turned off. The obtained silanidescan be used as building blocks for the construction of more extended
oligosilane systems or for the preparation of a geminal disilatranylsilane.
Experimental Section
General Remarks
All reactions involving air-sensitive
compounds were carried out under an atmosphere of dry nitrogen or
argon using either Schlenk techniques or a glovebox. Reagent grade
CHCl3 was used for the synthesis of chlorosilatrane 1. All other solvents were dried using a column-based solvent
purification system.[47] Ethyltris(trimethylsilyl)silane,[31] isopropyltris(trimethylsilyl)silane,[48] phenyltris(trimethylsilyl)silane,[48] 2,2-bis(trimethylsilyl)octamethyltetrasilane,[42] (tert-butyldimethylsilyl)tris(trimethylsilyl)silane,[31] 1-chloro-3,3-bis(trimethylsilyl)heptamethyltetrasilane,[19] and 1,2-dichlorotetramethyldisilane[49,50] were prepared according to previously published procedures. Methyltris(trimethylsilyl)silane[51] was prepared similarly to ethyltris(trimethylsilyl)silane[31] by reaction of tris(trimethylsilyl)silyl potassium
with dimethyl sulfate. All other chemicals were obtained from different
suppliers and used without further purification.1H (300 MHz), 13C (75.4 MHz), 19F (282.2 MHz),
and 29Si (59.3 MHz) NMR spectra were recorded on a Varian
INOVA 300 spectrometer and are referenced to tetramethylsilane (TMS)
for 1H, 13C, and 29Si and to CFCl3 for 19F. In the case of reaction samples a D2Ocapillary was used to provide an external lock frequency
signal. To compensate for the low isotopic abundance of 29Si, the INEPT pulse sequence[52,53] was used for the amplification
of the signal. Elemental analysis was carried out using a Heraeus
VARIO ELEMENTAR instrument. GC/MS analyses were carried out on a Agilent
7890A (capillary column HP-5MS; 30 m × 0.250 mm; film 0.25 μm)
with an Agilent 5975C mass spectrometer.
X-ray Structure Determination
For X-ray structure analyses
the crystals were mounted onto the tip of glass fibers, and data collection
was performed with a BRUKER-AXS SMART APEX CCD diffractometer using
graphite-monochromated Mo Kα radiation (0.71073 Å). The
data were reduced to Fo2 and
corrected for absorption effects with SAINT[54] and SADABS,[55] respectively. The structures
were solved by direct methods and refined by full-matrix least-squares
methods (SHELXL97).[56] If not noted otherwise,
all non-hydrogen atoms were refined with anisotropic displacement
parameters and all hydrogen atoms were located in calculated positions
to correspond to standard bond lengths and angles. Crystallographic
data (excluding structure factors) for the structures of compounds 3, 5–7, 9–11, 14, and 17–19 reported in this paper have been deposited with the Cambridge Crystallographic
Data Center as supplementary publication nos. CCDC 1062942 (3), 1062948 (5), 1062943 (6), 1062944
(7), 1062946 (9), 1062945 (10), 1062951 (11), 1062947 (14), 1062941(17), 1062949 (18), and 1062950 (19). Data can be obtained free of charge at http://www.ccdc.cam.ac.uk/products/csd/request/.Figures of solid-state molecular structures were generated
using Ortep-3 as implemented in WINGX[57] and rendered using POV-Ray 3.6.[58]
N(CH2CH2OSiMe3)3
To a
solution of triethanolamine (10.0 g, 0.067 mol) in
dichloromethane (100 mL) in a 500 mL two-neck flask was added triethylamine
(30.0 g, 0.301 mol), and the mixture was cooled to 0 °C in an
ice bath. Within 1 h trimethylchlorosilane (25.5 g, 0.234 mol) was
added dropwise to the flask. After the ice bath was removed, the reaction
mixture was warmed to room temperature with stirring over 2 h. The
reaction mixture was then added slowly to water (100 mL), and the
organic phase was separated from the aqueous layer, which was washed
twice with small portions of dichloromethane. The combined organic
phases were dried over Na2SO4. The organic solvent
was removed under vacuum, and a pale yellow oil (18.0 g, 0.049 mol,
73%) was obtained as the product with spectroscopic properties in
accordance with reported data.[59] NMR (δ
ppm, CDCl3): 1H, 3.51 (t, J = 6.8 Hz, 6H, OCH2), 2.59 (t, J = 6.8
Hz, 6H, NCH2), 0.00 (s, 27H, SiMe3); 13C, 61.05 (OCH2), 57.59 (NCH2), −0.69
(Me3Si); 29Si, 17.6.
Silatranyl Chloride (1)
A mixture of N(CH2CH2OSiMe3)3 (14.0 g, 0.0383
mol) and SiCl4 (7.00 g, 0.0412 mol) was dissolved in chloroform
(40 mL) in a 250 mL three-neck flask with condenser. The reaction
mixture was stirred and heated for 6 h to reflux. After all volatiles
were removed under vacuum, the residue was washed with chloroform
and 1-chlorosilatrane (7.10 g, 0.0339 mol, 82%) was obtained as a
white powder with spectroscopic properties in accordance with reported
data.[60] NMR (δ ppm, CDCl3): 1H, 3.97 (t, J = 5.9 Hz, 6H, OCH2), 3.01 (t, J = 5.9 Hz, 6H, NCH2); 29Si, −85.9.
Silatranyl Triflate (2)
A slurry of 1-chlorosilatrane
(2.00 g, 9.54 mmol, 1.00 equiv) and trimethylsilyl triflate (4.24
g, 19.07 mmol, 2.00 equiv) in toluene (1 mL) was strongly stirred
and heated for 72 h to 65 °C. The progress of the reaction was
monitored by 1H NMR spectroscopic analysis of the peaks
of trimethylsilyl triflate and the formed trimethylchlorosilane. Compound 2 was obtained as an air-sensitive white powder (2.92 g, 9.50
mmol, 99%) after removing volatiles under vacuum. NMR (δ ppm,
DMSO-d6): 1H, 3.84 (t, J = 5.9 Hz, 6H, OCH2), 3.13 (t, J = 5.9 Hz, 6H, NCH2); 13C, 118.33 (q, J = 318 Hz, CF3), 57.52 (OCH2), 50.69 (NCH2); 29Si, −97.1; 19F, −77.45. Anal. Calcd for C7H12F3NO6SSi (323.31): C, 26.00; H, 3.74; N, 4.33;
S, 9.92. Found: C, 25.73; H, 3.54; N, 4.20; S, 9.69.
Tris(trimethylsilyl)silatranylsilane
(3)
Tetrakis(trimethylsilyl)silane (2.00 g,
6.23 mmol) and KOtBu (734 mg, 6.54 mmol) in THF (5 mL)
were stirred for 14 h. After
the formation of the organosilyl anion was confirmed by means of NMR
spectroscopy, the solvent was removed and toluene was added (5 mL).
To a solution of this compound was added a suspension of 2 (2.22 g, 6.85 mmol) in toluene (2 mL) dropwise within 2 h. After
12 h the precipitate was removed by filtration and washed with pentane
(3 mL) and then the solvent was removed. After sublimation (40 °C,
1 mbar) and recrystallization with hexanecolorless crystalline 3 (1.35 g, 51%) was obtained. Mp: 144–146 °C.
NMR (δ ppm, CDCl3): 1H, 3.65 (t, J = 5.6 Hz, 6H, OCH2), 2.72 (t, J = 5.6 Hz, 6H, NCH2), 0.15 (s, 27H, Me3Si); 13C, 58.56 (OCH2), 52.15 (NCH2), 2.20
(Me3Si); 29Si, −9.9 (Me3Si),
−52.6 (SiO3), −133.9 (Siq). NMR
(δ ppm, C6D6): 1H, 3.30 (t, J = 5.6 Hz, 6H, OCH2), 1.83 (t, J = 5.6 Hz, 6H, NCH2), 0.53 (s, 27H, Me3Si); 13C, 58.55 (OCH2), 51.53 (NCH2), 2.77
(Me3Si). Anal. Calcd for C15H39NO3Si5 (421.91): C, 42.70; H, 9.32; N, 3.32. Found:
C, 43.29; H, 8.62; N, 3.25. MS (70 eV) m/z (%): 423(3) [M– + H], 406(4) [M+ – Me], 278(3) [(SiMe3)3SiSiH3+], 249(1) [(SiMe3)3SiH],
232(2) [Si4Me8+], 174(100) [N(CH2CH2O)3Si+], 147(1) [N(CH2CH2O)3+], 73(13) [SiMe3+].
3 (350 mg, 0.75 mmol) and
KOtBu (87 mg, 0.77 mmol) were dissolved in THF (2 mL).
After 14 h the formation of the silyl anion 10 was confirmed
by means of NMR spectroscopy; the solvent was removed, and benzene
was added (3 mL). This solution was added dropwise to 1-chloro-3,3-bis(trimethylsilyl)heptamethyltetrasilane
(300 mg, 0.75 mmol) in toluene (3 mL) at 0 °C within 1 h. After
12 h the solvent was removed, the residue treated with pentane, and
the insoluble parts were filtered off. The solvent was again removed,
and recrystallization with diethyl ether/acetonitrile (1/1) afforded
colorless crystalline 16 (354 mg, 66%). Mp: 130–136
°C. NMR (δ ppm, CDCl3): 1H, 3.66
(t, J = 5.56 Hz, 6H, OCH2), 2.73 (t, J = 5.61 Hz, 6H, NCH2), 0.39 (s, 6H, Me2Si), 0.35 (s, 6H, Me2Si), 0.24 (s, 27H, 3 Me3Si), 0.20 (s, 18H, 2 Me3Si); 13C, 58.50 (OCH2), 51.84 (NCH2), 3.52 (Me3Si), 2.97
(Me3Si), 0.53 (Me2Si), 0.40 (Me2Si); 29Si, −9.2 (Me3Si), −9.6 (Me3Si), −30.6 (Me2Si), −30.8 (Me2Si), −53.8 (SiO3), −128.6 (Siq), −129.3 (Sq). Anal. Calcd for C25H69NO3Si10 (712.68): C, 42.13; H, 9.76;
N, 1.97. Found: C, 41.66; H, 9.65; N, 1.73. UV: λ 254 nm (ε
= 5.45 × 104 M–1 cm–1).
Authors: Clemens Krempner; Jürgen Kopf; Constantin Mamat; Helmut Reinke; Anke Spannenberg Journal: Angew Chem Int Ed Engl Date: 2004-10-11 Impact factor: 15.336
Authors: Walter Gaderbauer; Istvan Balatoni; Harald Wagner; Judith Baumgartner; Christoph Marschner Journal: Dalton Trans Date: 2009-12-10 Impact factor: 4.390
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