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ening observed in some spectra for certain telluronium-
OPPh3 complexes.
between the calculated chemical shielding and the measured
dTe for the telluronium-OPPh3 adducts (Figure S20). This was
expected because the measured dTe in solution corresponded
to an equilibrium process whereas the chemical shielding
were calculated for the adducts only.
It is interesting to note that the measured and calculated
chemical shift values of the telluroniums reported here nicely
fit with those recently reported (Figure S19).[24e]
To further probe this Ph3PO··Te interaction and to assess
the formation of a monoadduct Ph3PO–Te+, we performed
NOESY experiment (Figure S7) on the solution containing
Ph3PO and 3c, the most effective salt for such complex
formation (see above). This experiment clearly established
the spatial proximity of ortho protons of Ph3PO with the ortho
protons of the 3,5-di(trifluoromethyl)phenyl group of the
telluronium entity (Figure 2a). Furthermore, nOe was also
Therefore, electronic effect should best be detectable if no
competition for Te s-holes occurs. The telluronium series 1c,
2c, 3c and 4c, carrying the less coordinating anion BArF, was
designed and prepared for these reasons in order to maximize
Ph3PO··Te interaction. Rewardingly, these BArF derivatives
exhibited the largest NMR shifts (entries 3, 6, 9 and 15),
whatever the measured nucleus. Furthermore, good correla-
tions between Dd and s Hammett constants were obtained in
17O and 31P NMR (R2 = 0.9375 and 0.9846 respectively; see
Figure S4). The latter clearly confirms the formation of
Ph3PO··Te complexes, and the role electronic effects played
in this formation: the most effectively formed was obtained
with the more electrodeficient telluronium 3+, the one having
the largest s-holes (see Vs,max values above), inducing the
largest 17O and 31P NMR shifts.
Alternatively, the anion effect could be best evaluated
within the telluronium series which exhibits the largest s-
holes (see Table S21), that is, the 3+ derivatives. Interestingly,
the a index proposed by Alvarez to define the coordination
ability of anions toward transition metal ions[23a] allowed to
rationalize the observed Dd variations. Remarkable correla-
tions were indeed achieved with 17O and 31P NMR shifts for
the 3a-3 f telluronium salt series (entries 7–12; see Figure S5,
R2 = 0.9607 and R2 = 0.9420 respectively). These results
confirm that coordination of the telluronium counterions
compete with Ph3PO for the formation of Ph3PO··Te com-
plexes.
It is worth noticing that, although a values were reported
for transition metals, lanthanides, and s-block metals,[23] the
present correlations suggest that they are also well suited for
telluronium cations.
Figure 2. a) Representation of the interactions between OPPh3 and the
telluronium protons of 3c as suggested from 17O, 31P and 125Te NMR
and NOESY experiment (only one single hydrogen was highlighted for
clarity); b) B3LYP-D3/Def2TZVPP calculations of the 3+-Ph3PO com-
plex; c) mass spectrum of the 3+-Ph3PO complex.
In contrast to DdO and DdP, only moderate to poor
correlations could be achieved with DdTe, both for electronic
and anion effects (see Figure S6). This was expected because
125Te NMR spectroscopy is highly sensitive to electronic and
geometry changes in the tellurium environment.[24] Never-
theless, the correlation profile between DdTe and a for the
telluronium salt series 3+XÀ showed that DdTe is differently
influenced if the anion is well or poorly coordinating. Thus, by
considering only low (BArF and B(C6F5)4) and medium (SbF6
and BF4) coordinating anions, a very good correlation (R2 =
0.9931) was obtained between DdTe and a. With the more
coordinating anions (NO3 and TfO), the effect of Ph3PO
addition is balanced by other parameters, probably related to
their competition for interaction with the telluronium and
may be some modifications of the telluronium geometry if
both the anion and Ph3PO interact with.
detected between the ortho-protons of Ph3PO and the methyl
group of the telluronium. Interestingly, calculations per-
formed on a complex Ph3PO-3+ also highlighted the proximity
of these protons (Figure 2b and S25), with a very short
distance between Te and O (2.570 ꢁ), in line with the
strongest 17O NMR shift (Dd 21.1 ppm) observed with this
complex. Its formation was further confirmed by in situ mass
spectrometry, which allowed to detect the species present in
the corresponding solution with a mass peak at 849.0448
within a set of peaks typical for the isotopic distribution of
a 1:1 adduct between 3c and Ph3PO (Figure 2c and S8).
Overall, these effects established the presence of a ChB
between Te and O of Ph3PO through interaction of the latter
with the aryl-Te s-hole located between the telluronium
methyl and the other aryl group, as schematically shown in
Figure 2a.
A complementary analysis of 125Te chemical shifts was
performed by calculating the chemical shielding of the
tellurium in telluronium cations 1+-4+ (see S. I., section
VII). Interestingly, the good linear correlation between the
chemical shifts of telluroniums 1c–4c measured in solution
and the calculated chemical shielding of 1+-4+ showed that the
dTe trend in this series can be well reproduced by DFT
calculations (R2 = 0.9076, Figure S18). This result confirmed
that dTe in telluroniums 1c–4c is mostly influenced by
electronic parameters. However, no correlation was observed
As these observations clearly showed the Lewis acidity of
the cationic chalcogen and its ability to activate a carbonyl-
type derivative, it was worth evaluating their propensity to act
as catalyst in some reactions. The bromination of anisole with
N-bromosuccimide (NBS) was first used as benchmark
reaction with catalysts 1–3 (Table 2). Interaction of the NBS
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Angew. Chem. Int. Ed. 2021, 60, 2 – 8
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