ChemComm
Communication
Fig. 4 (A) CDS of MB and a-CD included Na–Azo-POM (3 : 5 : 5 in molar
ratio) in aqueous solution by gradually increasing the concentration of
NaCl to 0, 0.043, 0.086, 0.128, 0.171, 0.214, 0.257, 0.342, 0.428, 0.599,
0.770, 1.112, and 1.454 mmol mlÀ1. (B) CDS of MB, Na–Azo-POM mixed
with a-CD in aqueous solution by gradually increasing the temperature
(20, 30, 40, 50, 60, and 80 1C).
Fig. 3 UV-Vis spectra of (a) MB (3.0 Â 10À5 mmol mlÀ1), (b) MB mixing
with Na–Azo-POM and a-CD, and (c) Na–Azo-POM mixed with a-CD in
aqueous solution (MB : a-CD : Na–Azo-POM at molar ratio of 3 : 5 : 5).
As shown in Fig. 3, when MB cations are added into the a-CD
included Azo-POM solution, the absorptions at ca. 627 and 713 nm
with a broad band decreased markedly at 560 nm, to the visible
region. The bands moving to the long wavelength in comparison to
isolate MB point out the electrostatic interaction-induced MB aggre-
gation around POMs.10 In contrast, the band at 345 nm that is
ascribed to the absorption of Azo group does not show any change
in its state without MB, indicating a constant inclusion state.
To confirm the chiral induction and migration, CDS of the
three-component system were carried out (Fig. S11, ESI†). For the
MB mixed with Na–Azo-POM, no chiral signal was found. When
MB was mixed with a-CD, the chiral signal of MB molecule could
still not be seen due to the bigger size of MB. The 2D ROESY NMR
spectrum also confirms that no inclusion of a-CD to MB occurring
through b-CD works well (Fig. S12, ESI†). In contrast, when the
three components are mixed together, on one hand, a positive
Cotton signal at around 345 nm and a negative signal at about
440 nm can be well ascribed to the host–guest recognition-induced
chirality of the p–p* transition band of trans-azobenzene groups.
On the other hand, the positive Cotton signals at 558 and 720 nm
and much stronger negative Cotton signal at 629 nm appear and
can be unequivocally attributed to the induced chirality of MB.
These results concerning Cotton activity clearly prove the chiral
migration from a-CD to MB bridged by Azo-POM.
Apparently, both electrostatic interactions and host–guest
recognition play crucial roles in the chiral migration and can be
used for modulating the chirality of Azo-POM and the MB dye
molecule. With the addition of sodium chloride in the three-
component system, the intensity of Cotton signals of MB
obviously decreases until the concentration of the salt reaches
ca. 1.45 mmol mlÀ1 (Fig. 4A). It is well known that the existence of
electrolytes can increase the ionic strength of the solution system,
which weakens the electrostatic interaction of ionic pairs.11 As a
result, the interaction between Azo-POM and MB fades gradually
so that the average distance between the cationic dye and the
anionic cluster becomes greater. Nevertheless, the ionic pair could
not be completely decomposed by simply adding electrolytes.
When the concentration of NaCl was gradually increased, the
chemical shifts of MB in Na–Azo-POM-mixed solution moved
close to those of isolated MB solution, indicating the weakening
of the electrostatic interaction (Fig. S13, ESI†). In addition, based
on the comparison of the absorption spectra (Fig. S14, ESI†), the
fact that the bands of MB that are assigned to the aggregation
state shift to the long wavelength demonstrates the increase in the
amount of dissociated MB with the addition of salt. This change
also implies that the chiral transfer from Azo-POM is blocked by
weakening electrostatic interactions. As seen from the same CDS
measurement in Fig. 4A, the intensity of the chiral signal of Azo
group at 345 nm increases with the addition of salt, indicating
that the host–guest recognition is enhanced by the ionic strength
change. In contrary, when heating the three component system,
accompanying by the decrease of chiral signals of MB, we also see
the decrease of chiral intensity of Azo group at 345 nm (Fig. 4B).
Normally, the host–guest recognition can be broken down under
higher temperature. This change implies that the host–guest
interaction is gradually dissociated, and consequently, the inten-
sity of chiral signals of MB decreases greatly at the same time.
1
Variable-temperature H NMR spectra indicate constant electro-
static interaction between MB and Azo-POM cluster while increas-
ing temperature (Fig. S15, ESI†). Therefore, it is reasonable to
think that the chiral transfer is stopped by the decomposition
between the a-CD and Azo-POM during the heating process.
A new single-side azobenzene-modified Anderson-type POM was
synthesized. The novel umbrella-like hybrid cluster displays inter-
esting property when building a three component supramolecular
system with a-CD and MB dye cations via both host–guest recogni-
tion and electrostatic interactions. The chirality of a-CD is amplified
into Azo-POM and MB cations. Furthermore, the chiral migration is
modulated through simply tuning the concentration of electrolyte
and heating. The present results open a new approach to drive
POMs as inorganic bridging ligands for chiral transfer and
amplifications to cationic molecules.
This work was financially supported by the National 973 Program
(2013CB834503), NSFC (91227110, 21221063), Ministry of Education
of China (20120061110047), and open project of SKL-PPC, CAS.
Notes and references
1 A. Proust, B. Matt, R. Villanneau, G. Guillemot, P. Gouzerh and
G. Izzet, Chem. Soc. Rev., 2012, 41, 7605.
2 (a) W. Bu, H. Li, H. Sun, S. Yin and L. Wu, J. Am. Chem. Soc., 2005,
127, 8016; (b) Y. Han, Y. Xiao, Z. Zhang, B. Liu, P. Zheng, S. He and
W. Wang, Macromolecules, 2009, 42, 6543; (c) B. Hasenknopf,
R. Delmont, P. Herson and P. Gouzerh, Eur. J. Inorg. Chem., 2002,
1081; (d) C. Yvon, A. J. Surman, M. Hutin, J. Alex, B. O. Smith,
This journal is ©The Royal Society of Chemistry 2014
Chem. Commun., 2014, 50, 10823--10826 | 10825