Separable Pseudo[n]rotaxanes
FULL PAPER
the steric interactions will also prevent two CB[7] rings from
threading onto two adjacent p-xylene units. If this self-as-
sembling mode is also applicable to the higher order oligoal-
kylammonium salts, one can expect that at the maximum
degree of threading, pseudo[3]rotaxane, pseudo[4]rotaxane,
ure 4D). The pure pseudo[3]rotaxane again was obtained by
simple counterion exchange with NH4PF6, and it was also in-
teresting that the sample had a higher solubility in acetoni-
trile than the pseudo[2]rotaxane obtained from 2·ACHTUNGTRENNUNG(PF6)3,
probably because there were two CB[7] units encircling the
1
and pseudo[5]rotaxane will be formed for 3·
and 5·(PF6)8, respectively.
To further confirm this assumption and to understand the
exact self-assembling mode, threading of 3·(PF6)4, 4·(PF6)6,
and 5·(PF6)8 with CB[7] was conducted using a similar ap-
A
N
cationic thread. H NMR spectra of the pure pseudo[3]ro-
N
taxane in acetonitrile clearly supported such a self-assem-
bling mode (Figure 2B). In addition, the HR-ESIMS exhib-
À
A
U
ited three peaks at m/z 676.10 for [MÀ4PF6 ]4+, 949.83 for
À
À
E
[MÀ3PF6 ]3+ and 1497.08 for [MÀ2PF6 ]2+ (Figure 1C),
further confirming the proposed structure. Based on these
results, it will be natural to expect that the threading of 4·
proach. In all cases, a gentle heating of the solution was
needed to obtain clear solutions. Upon addition of various
amounts of CB[7], the resonances of 34+ experienced a simi-
lar upfield and downfield shift (Figure 4). When four equiv-
ACHUTNGRENU(NG PF6)6 and 5·AHCTUNGTERN(NGUN PF6)8 with excess CB[7] will lead to the forma-
tion of pseudo[4]rotaxane and pseudo[5]rotaxane with the
CB[7] rings located at specific sites. In fact, our experimen-
tal data did support this assumption. The threading of 4·
(PF6)8 with CB[7] was followed by 1H NMR
ACHUTNRGEN(NUG PF6)6 and 5·ACHTUGNTRENNUGN
spectroscopic measurements (Figures S2 and S3 in the Sup-
porting Information). In both cases, a large excess of CB[7]
was required to reach a maximum degree of threading, and
finally, simple NMR spectra were obtained that can be as-
signed to the highly symmetric pseudo[4]rotaxane and pseu-
do[5]rotaxane, respectively. It was clear that for 4·
three CB[7] molecules were located at the two terminal and
one central xylene units. Similarly for 5·(PF6)8, four CB[7]
ACHTUNGTRENNUNG(PF6)6,
AHCTUNGTRENNUNG
molecules are located along the cationic thread with one un-
complexed xylene unit bridged between neighboring CB[7]
rings (see the models in Figures 1 and 2). Such a self-assem-
1
bling mode was further proved by the H NMR spectroscop-
ic and HR-ESIMS measurements of the pure pseudo[n]ro-
taxanes, which were obtained by similar counterion ex-
1
change. As shown in Figure 2, simple H NMR spectra were
obtained for the pseudo[4]rotaxane in CD3CN and it was in
agreement with the proposed structure (Figure 2C). The col-
lection of the 1H NMR spectra of the pseudo[5]rotaxane
was a little more challenging because of its poor solubility.
1
After a long time, a relatively clear H NMR spectrum was
Figure 4. 1H NMR spectra (500 MHz, CF3COOD/D2O=1:1, 298 K) of
obtained, which again supported our expectation (Fig-
ure 2D).[30] The HR-ESIMS measurements further proved
the formation of these pseudo[n]rotaxanes (Figure 1D, E).
A) CB[7], B) 3·
G
N
ACHTUGNERTN(NUNG PF6)4 =2:1,
E) CB[7]/3·(PF6)4 =3:1, and F) CB[7]/3·ACTHUNGTRENNUNG
A
The mass spectrum of the pseudo[4]rotaxane formed from
À
alents of CB[7] were added, a simple 1H NMR spectrum
was obtained that clearly showed that a symmetric pseu-
do[3]rotaxane had formed, in which the two CB[7] rings en-
circled the two terminal xylene units with the central xylene
unit uncomplexed (Figure 4F). As a result, the resonances
for the complexed phenyl rings (Hb, Hc) showed an upfield
shift to d=6.89 (doublet) and 6.77 ppm (doublet), and the
resonance for the central uncomplexed phenyl rings (Hf)
displayed a downfield shift to d=8.02 ppm as a singlet. Sim-
ilar changes were observed for the methylene protons of 34+
and the integration ratio between the two sets of resonances
showed the expected value of 2:1. We also found that to
reach a maximum degree of threading, an excess of CB[7]
had to be added, as one can see that the addition of two
equivalents of CB[7] resulted in an equilibrium of both
pseudo[3]rotaxane and pseudo[2]rotaxane in solution (Fig-
4·
G
,
À
À
850.54 for [MÀ5PF6 ]5+, 1099.43 for [MÀ4PF6 ]4+ and
À
1514.23 for [MÀ3PF6 ]3+; the pseudo[5]rotaxane from 5·
À
A
,
808.17 for [MÀ7PF6 ]7+, 967.06 for [MÀ6PF6 ]6+, 1189.52
À
À
À
À
for [MÀ5PF6 ]5+ and 1524.24 for [MÀ4PF6 ]4+. All the
peaks gave well-resolved isotope distributions in agreement
with the calculated values.
Conclusions
In conclusion, a series of well-defined, higher order pseu-
do[n]rotaxanes (n=2, 3, 4, 5) have been prepared in pure
form by using a simple “threading-followed-by-precipita-
tion” approach. To the best of our knowledge, the obtained
Chem. Eur. J. 2009, 15, 6050 – 6057
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6055