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with Me3SiCF2H,[7b] stoichiometric amounts of CsF and
tBuOK were initially tested as the activators. However, only
the signals of CF2H2 and unreacted Me3SiCF2H were detected
by 19F NMR spectroscopy at a wide range of temperatures
(À708C to room temperature). The failure to observe any
pentacoordinate difluoromethyl silicate species probably
À112.1 ppm) versus Me3SiCF3 (d = 5.4 ppm).[5a] In the
1H NMR spectrum, both the signals of the CF2H (d =
5.00 ppm) and Me (d = À0.24 ppm) groups are also detected
to be upfield compared with those of Me3SiCF2H [d(CF2H) =
1
5.85 ppm; d(Me) = 0.14 ppm]. The JH-F coupling constant is
in good agreement with the corresponding coupling observed
in 19F NMR [d = À130.0 ppm (d, 1JH-F = 47.3 Hz)]. According
to the ratio (2:9) of integrated area of the 1H NMR signals of
CF2H and Me, we inferred that the above silicon species is
À
arises from the strong affinity of the HCF2 to the alkali-
metal cations, and thus leads to a spontaneous decomposition
of the difluoromethyl silicates into HCF2À, with subsequent
protonation by either adventitious water or the solvent THF.
Considering that the countercation effect can significantly
influence the stability of hypercoordinate silicate anions,[3f,5b]
we turned our attention to the employment of a crown
ether[12] as an additive to stabilize the silicate intermediate by
À
a pentacoordinated bis(difluoromethyl)slicate with five Si C
bonds, that is, [(18-crown-6)M]+[Me3Si(CF2H)2]À (M = Na, K,
Cs).[16] The observed quintet peak in 29Si{1H} NMR spectrum
supports a trigonal-bipyramidal structure with two axial CF2H
groups and three equatorial methyl groups, and it is similar to
the structure of [Me3Si(CF3)2]À.[5a] Moreover, the 13C NMR
À
minimizing the interaction between HCF2 and the alkali
1
metal cations (Scheme 1b). To our delight, a weak signal at
around d = À130.0 ppm was observed by 19F NMR spectros-
copy at room temperature using the combination of CsF/18-
crown-6 as the activator (see Figure S1 in the Supporting
Information). Much stronger signals with the similar chemical
shifts were observed at temperatures ranging from À788C to
room temperature when the combinations of more soluble
tBuOK/18-crown-6, tBuOCs/18-crown-6, and even tBuONa/
18-crown-6 were used. Compared with the 19F NMR chemical
shift of Me3SiCF2H (d = À140.7 ppm), the downfield shift of
the observed signal is likely to correspond to an anionic
species.[13] To determine the structure of the observed species,
we further carried out 29Si{1H} NMR, 13C{1H} NMR,
1H NMR, and heteronuclear multiple quantum coherence
(HMQC) experiments of the reaction between Me3SiCF2H
and tBuOCs/18-crown-6 in [D8]THF (Figure 1; see Figur-
signals of CF2H [d = 140.3 ppm (t, JC-F = 285 Hz)] and Me
(d = À3.2 ppm), which were assigned by 1H-13C HMQC
analysis, appear downfield from those of Me3SiCF2H
[d(CF2H) = 123.7 ppm
(t,
1JC-F = 253 Hz);
d(Me) =
À6.5 ppm]. An increase in 1JC-F coupling as well as a decrease
2
in JSi-F coupling, which have been observed in the trans-
formation of Me3SiCF3 into [Me3Si(CF3)2]À,[5a] are probably
characters of bipyramidal [R3Si(Rf)2]À species with two Rf
groups at the axial positions.
It is noteworthy that these pentacoordinate silicates were
relatively stable below À308C and decomposed gradually to
CF2H2 when slowly raising the temperature from À308C to
208C [for variable-temperature (VT) NMR study, see Figur-
es S7 and S17]. Moreover, [Me3Si(CF2H)2]À was the only
detectable difluoromethylated hypercoordinate silicon spe-
cies regardless the ratio of Me3SiCF2H/tBuOM (either > 1:1
or not). We also attempted to observe CF2HÀ at a wide range
of temperatures (from À788C to 208C), but no evidence
supported the persistence of this species in our system, which
À
is significantly different from the CF3 anion derived from
Me3SiCF3.[5c] The generation of CF2HD and CF2H2 as side
products when using [D8]THF as the solvent indicates that
CF2HÀ is kinetically unstable and has a high tendency to
abstract a proton from both THF and 18-crown-6 (see
Figures S3 and S13).
Having identified the relatively stable intermediate
[Me3Si(CF2H)2]À, we next sought to probe its reactivity in
nucleophilic difluoromethylation reactions. The experiment
was conducted by adding the electrophilic substrate to a THF
solution of [Me3Si(CF2H)2]À pre-generated from stoichiomet-
ric amounts of tBuOM (M = Na, K, Cs), 18-crown-6, and
Me3SiCF2H in a molar ratio of 1:1:2. To our surprise,
enolizable ketones, which are challenging substrates under
previously reported difluoromethylation conditions,[7a,b,d] can
be readily difluoromethylated. Thus, the reaction between 1-
(2-methoxyphenyl) ethanone (1i) and [Me3Si(CF2H)2]À, gen-
erated from tBuOCs/18-crown-6/Me3SiCF2H, gave the corre-
sponding difluoromethylated alcohol in good yield (Sche-
me 2a; for details see Figure S8). However, when tBuONa
was used instead of tBuOCs, the pre-generated [Me3Si-
(CF2H)2]À failed to undergo addition to 1i, only affording
CF2H2 as the detectable side product. Based on these results,
we concluded that the countercation effect not only influen-
ces the stabilization of [Me3Si(CF2H)2]À, but it also dramat-
Figure 1. 29Si{1H} NMR (a) and 1H NMR (b) spectra of [Me3Si-
(CF2H)2]À, generated from tBuOCs/18-crown-6 and Me3SiCF2H in
[D8]THF at À308C. In (a), the signals (*) at d=7.5–7.0 ppm are
assigned to Me3SiOtBu as well as side-products arising from the
silylation of [D8]THF and 18-crown-6.
es S2–S6 and Table S1).[14] In the 29Si{1H} NMR spectrum, the
2
signal is shifted upfield [d = À118.4 ppm (quint, JSi-F
=
10.3 Hz)] compared with that of Me3SiCF2H [d = À0.04 ppm
2
(t, JSi-F = 28.8 Hz)], and is in accordance with the formation
of a pentacoordinated silicate species.[15] This chemical shift
change is similar to that of the reported [Me3Si(CF3)2]À (d =
2
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Angew. Chem. Int. Ed. 2016, 55, 1 – 6
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