responding to external stimuli, and may extend over the
modulation of other properties such as electronic (redox
modifications, conductivity), magnetic, and mechanical. The
dynamic polymers are illustrative of the potential offered by the
application of the principles of constitutional dynamic chemis-
try1,4,10 to materials science.
Notes and references
{ Equimolar amounts of the corresponding bis-hydrazine (compounds L
and P, ESI{) and the dialdehyde monomers at concentrations around
0.04 M each were dissolved in the mixture of CHCl3 and THF (8 : 2 in
volume ratio; for the polymer P1) or CHCl3 (for the polymers P2, P3),
followed by addition of pentadecafluorooctanoic acid in 0.1 molar ratio
with respect to the resulting total hydrazone bonds. The solution was
heated at 60 uC for 12 h, then poured into a petri dish of 50 mm diameter
made of fluoroplastic, followed by evaporation at 60 uC at normal pressure
until most of the solvent had disappeared and then kept at 60 uC in vacuo
for 12 h. About 200 mg of the total amounts of monomers were used to
obtain polymer film of around 0.04–0.06 mm thickness.
Fig. 6 Cross-sectional schematic representation of the superimposition
of two hydrazone polymer layers.
§ Polymer thin layers were prepared using a 2 wt% THF solution of the
polymer by spin-coating onto 5 cm square quartz plates, which were rinsed
with acetone prior to use. The spin-speed and the period were 500 rpm and
60 s, respectively. These layers were subsequently dried in vacuo at 60 uC for
12 h.
1 J.-M. Lehn, Prog. Polym. Sci., 2005, 30, 814.
2 L. Brunsweld, B. J. B. Folmer, E. W. Meijer and R. P. Sisjbesma, Chem.
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3 (a) J.-M. Lehn, Polym. Int., 2002, 51, 825; (b) Supramolecular Polymers,
ed. A. Ciferri, Taylor & Francis, Boca Raton, 2nd edn, 2005; (c)
J.-M. Lehn, in Supramolecular Polymers, ed. A. Ciferri, Taylor &
Francis, Boca Raton, 2nd edn, 2005, ch. 1, p. 3.
Fig. 7 Fluorescence emission spectra of the overlapping domain of neat
hydrazone polymer films P1 and P2 under excitation at 425 nm as a
function of heating time.
4 (a) S. J. Rowan, S. J. Cantrill, G. R. L. Cousins, J. K. M. Sanders and
J. F. Stoddart, Angew. Chem., Int. Ed., 2002, 41, 898; (b) P. T. Corbett,
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12 In addition to the four ‘‘symmetrical’’ domains present in P1–P4, the
blend may also contain ‘‘unsymmetrical’’ domains having different
components on each side.
13 J.-M. Lehn, in Supramolecular Science: Where It Is and Where It Is
Going, ed. R. Ungaro and E. Dalcanale, Kluwer, Dordrecht, The
Netherlands, 1999, p. 287.
A detailed study on the emergence of fluorescence at the
interface was performed with two thin layers (average thickness of
about 0.15–0.2 mm, determined by a stylus method) of dynamers
P1 and P2 coated on a quartz plate§, which were superimposed
face-to-face (Fig. 6) and heated to 120 uC in an oven under a
stream of argon. The fluorescence intensity of the overlapping part
around 450–600 nm, measured on the layers, increased with
heating time in a manner similar to the case of the polymer blend
(Fig. 7). The result indicates that hydrazone bond exchange and
component migration occurred by heating through the interface of
the polymer layers P1 and P2, leading to expression of
fluorescence along with conjugation extension between the
hydrazone moieties.
In conclusion, the present results show that color and
fluorescence of polyhydrazone dynamers can be modified by
hydrazone bond exchange and component recombination. They
also demonstrate that such processes can occur even at the
interface of two different polymer films, resulting in chemical
interconnection of the films. This feature has promising potential
for implementation in optical materials for systems such as
molecular sensing or photoactive devices. It gives access to
smart and adaptive dynamic materials1,10,13 controlled by and
4362 | Chem. Commun., 2007, 4360–4362
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