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this type of self-assembly process should lead to the formation of
catenanes in a thermodynamically controlled fashion.
11.5.1
[2]Catenanes
II
II
In this way, Pd
and Pt
hybrid [2]catenanes were assembled
from ligand
(Scheme 11.2) [30]. The diffusion
coefficients obtained from DOSY experiments of catenane
BPP34C10
⊂
M3a
L3
and
BPP34C10
showed that the
catenane are significantly larger than their components. The signals
from the ligand, macrocycle
·5NO
and ligand
L3
·3NO
3
3
II
complex showed
the same diffusion coefficients, indicating that the three components
diffuse as a whole. In the [2]catenane, exchange between the “inside”
and “alongside” hydroquinol rings is slow at room temperature,
resulting in all of the OCH
BPP34C10
, and the Pd
1
groups being anisochronous on the
H
2
1
13
C NMR spectra showed the upfield shift
of the signals for the “inside” hydroquinol ring protons and carbons
as a result of the π-π
NMR time scale. The
H and
stacking and [C-H
π] interactions with the
pyridine and
-phenylene rings on the short side of the rectangle. The
protons and carbons of these rings are shifted downfield from those
of the macrocycle
p
. Moreover, the signals for the protons
and carbons at the central positions of the bipyridine moieties have
shifted upfield as a result of the shielding effect of the macrocycle
BPP34C10
M3a
·5NO
3
.
Scheme 11.2
Synthesis of catenanes
BPP34C10
⊂
M3a,b
·5NO
.
3
Employing the same strategy that we used for the preparation of
catenane
BPP34C10
⊂
M3a
, the analogous platinum catenane
could be isolated as its hexafluorophosphate salt in high yield (85%).
·5NO
3
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