Angewandte
Communications
Chemie
the tubes with a layer repulsive to the anions, and thus
provided corroborative support for operational anion–p
interactions, i.e., the existence of anion–p catalysis on
MWCNTs (entries 5–7, 9–10, and 12–13).
SWCNTs 9s were with A/D = 6.8 less active than
MWCNTs 9m with A/D = 25 (Figure 2, blue, entries 5, 17)
but could be further inactivated by p-basic competitor 12
(Figure 2, pink, entries 17 and 18). This significant difference
is interesting because it supports that transition states on the
surface of MWCNTs could be stabilized by polarizability
along the tubes but also between the layers, somehow
combining previously explored through-bond contributions
from very large p surfaces beyond fullerenes on the one hand
and from through-space synergistic anion-(p) -p interactions
n
[
3]
on p-stacked foldamers on the other hand (Figure 1b).
[
3]
The binding of anion–p catalyst 9n (Scheme S1) on the
surface of unmodified MWCNTs 7m increased their activity
by maximal DA/D =+ 7.1 (Figure 2, entry 22; Figure 3e, blue
+). The coinciding increase in rate and selectivity with
MWCNT concentrations supported that the central principles
of catalysis also apply for these more complex systems, in this
case increasing transition-state recognition on the naphthale-
nediimide (NDI) surface in 9n by electron sharing with the
carbon nanotubes 7m (Figure 3e, turquoise ~). Activation of
Figure 3. a) Product formation (A, 3, blue
&
; D, 4, blue &) with 9m as
a function of time (10 mol%, 200 mm 1, 10 equiv 2, [D ]THF/CDCl
:1). b) Normalized A/D values with 9m as a function of the concen-
8
3
fullerene anion–p catalysts 9 f was, with up to DA/D =+ 1.4,
1
much weaker perhaps because the convex fullerenes prefer to
tration of inactivators 12 (pink !) and 13 (red !). For calibration, A/D
of TEA in 12 or 13 were used as A/Drel =0. c) A/D with 9m (blue *)
and TEA (pink x) (40 mm of tertiary amine) as a function of the
concentration of substrate 1. Equivalents of 2 were kept constant.
d) A/D with 9m (blue *) and TEA (pink x) as a function of their
[
21]
hide in the concave interior of carbon nanotubes (Figure 2,
entry 23; Figure 3 f, blue ~).
[
17]
The binding of the newly synthesized p-basic pyrene 9p
Scheme S1) by face-to-face p stacking on MWCNTs 7m
(
concentration (200 mm 1, 10 equiv 2). e) DA/D (A/DÀA/D , blue +)
0
slightly increased activity (up to DA/D =+ 1.2, Figure 2,
entry 20; Figure 3 f, red ~). Contrary to 9n, however, catalysis
and conversion after 4 days (turquoise ~) with 9n (5 mol%) as
a function of the concentration of activator 7m (wt% of the reaction
mixture). f) DA/D with 9 f (blue ~), 9p (red ~), 10p (red ~) and TEA
pink x) (5 mol%) as a function of the concentration of activator 7m
with 9p on 7m is unlikely to take place on the more repulsive
pyrene surface. This system thus documented the possibility
of non-covalent interfacing for anion–p catalysis on unmodi-
fied nanotubes 7m, although the obtained activities were
rather weak compared to covalent interfacing in 9m
(Figure 2, entry 20). As with covalent interfacing in 10m,
activities decreased with spacer elongation in the comple-
mentary non-covalent pyrene interfacer 10p on 7m (Figure 2,
entry 21; Figure 3 f, red ~). TEA, without p–p interfacer, was
(
(
wt% of the reaction mixture).
°
and decarboxylation reactions (DGTS ) were compared to
that observed with TEA to give differential transition-state
[3]
°
À1
stabilization DDGTS = À3.1 kJmol (Figure 2). Decreas-
°
À1
°
ing DDGTS = À2.3 kJmol
for 10m and DDGTS =
À1
À2.2 kJmol for 11m reproduced trends from A/D values
very well (blue, entries 5, 9, and 12).
the least sensitive to the presence of MWCNTs 7m (Figure 2,
entry 19; Figure 3 f, pink x).
Comparing bi- against unimolecular transformations, A/D
values increased with substrate concentration (Figure 3c).
They also increased with the concentration of catalyst 9m but
not with TEA (Figure 3d). Saturation behavior characterized
by a formal EC = 11 mm supported the presence of active
sites on MWCNTs, although the complex heterogeneous
system complicates interpretations, a call for caution that
naturally applies for all that follows.
In 1-chloronaphthalene 12, activities of 9m–11m
decreased (Figure 2, pink, entries 7, 10, and 13). Hill analysis
of the dose–response curve gave an IC = 5.9m for the
inactivation of catalyst 9m by 12 (Figure 2, entry 7; Figure 3b,
pink !; Table S2). Stronger inactivation was found for the
In summary, we provide experimental support for the
existence and significance of anion–p catalysis on carbon
nanotubes. Highlights include MWCNTs outperforming
SWCNTs owing to electron sharing within and between the
tubes, thus driving induced anion–p interactions from polar-
izability to the extreme, or the activation of existing anion–p
catalysts on the surface of pristine MWCNTs. The amphoteric
5
0
[12]
nature of MWCNTs suggests that, contrary to results from
[
6]
p-stacked foldamers, the above-mentioned insights should
hold also for the more conventional stabilization of cationic
intermediates on most polarizable p surfaces, i.e., induced
5
0
[
22]
cation–p rather than anion–p catalysis. Additional contri-
butions from the reduced dimensionality in 1D sliding
kinetics to anion–p catalysis, obviously most inviting on
[
20]
more p-basic 1,7-dialkoxynaphthalene (DAN)
a liquid at room temperature (IC = 2.6m, Figure 2, entry 6;
Figure 3b, red !). These results indicated that the p-basic 12
and 13 inactivate the catalysts by covering the p surfaces of
13, also
5
0
[
23]
carbon nanotubes, could deserve future attention.
The
heterogeneous nature of MWCNT anion–p catalysts is
Angew. Chem. Int. Ed. 2019, 58, 1 – 5
ꢀ 2019 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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