C O M M U N I C A T I O N S
transparent for more than 2 weeks at 60 °C, pH 7.2, showing good
colloidal stability of SNSs. In contrast, a small amount of F127 (x )
formation of 1D chains was induced by the transition from spherical
to wormlike micelles of the block copolymer, which also occurred
in the absence of Au nanoparticles. However, in our system, only
F127 aggregates with an average size of 30 nm can be detected by
dynamic light scattering (Figure S5). This size is comparable to
that of the typical spherical micelles of F127 reported by others.
It appears that a synergistic effect of F127 and silica nanoparticles
is contributing to the 1D assembly.
In conclusion, we have demonstrated a facile method to prepare
a 1D chain-like structure of silica nanospheres by using an
amphiphilic block copolymer. The anisotropy of chain-like assembly
can be fine-tuned using various handles like pH, ionic strength,
and temperature. This work may lead to new applications for silica
colloids and may provide useful ideas for the design of other
functional materials. Systematic investigation on the role of polymer
additives is now under progress.
0.1) strongly facilitates particle connection; precipitates consisting of
highly aggregated SNSs are generated right after the pH adjustment
to 7.2 (Figure S2a). The increase in the concentration of F127 results
in the formation of networked SNSs at x ) 0.5 (Figure S2b) and more
ordered 1D chains at x ) 0.8-2.0. Malmsten et al. reported that silica
nanoparticles of 15 nm in size aggregated in a dilute aqueous solution
2
2
19
of F127, but the formation of the anisotropic assembly has never
been reported.
The mode of particle assembly is controlled systematically by
changing the pH of the suspension. SNS colloids were mixed with
F127 (SiO /F127 ) 1:1 (w/w)) and incubated at 60 °C for 7 days
2
at various pHs ranging from 8.0 to 6.0. SNSs remain dispersed in
the suspension at pH 8.0, and only dispersed SNSs are observed
when transferred to a substrate (Figure 2a). In contrast, 1D chains
with relatively unbranched, straight structures are formed at pH
Acknowledgment. We thank Prof. Yukio Yamaguchi (The
University of Tokyo) for zeta potential and dynamic light scattering
measurements. We also gratefully acknowledge support from the
National Science Foundation (CMMI-0707610). Cryo-TEM char-
acterization was carried out at the Minnesota Characterization
Facility which receives support from the NSF through the National
Nanotechnology Infrastructure Network.
7
.5 (Figure 1d). Longer, more bent chains with branches are
observed at pH 7.0 (Figure 2b). Further lowering of pH to 6.0 gives
a more disordered chain-like assembly with increased branching
(
Figure 2c). The tendency of random assembly at lower pH can be
explained by the reduction of electrostatic repulsion between the
particles. The decrease in pH increases the number of undissociated
1
silanol groups on the silica surface and consequently reduces the
surface charge of SNSs (the zeta potentials of SNSs without F127
are -50.2, -44.2, -40.7, and -29.0 mV at pH 8.0, 7.5, 7.0, and
Supporting Information Available: Detailed experimental proce-
dures and Figures S1-S5. This material is available free of charge via
the Internet at http://pubs.acs.org.
6
.0, respectively). The undissociated silanols also facilitate the
1
9
interaction of PEO and SNSs through hydrogen bonding, which
may affect the adsorption of F127 on silica. The effect of pH on
the surface charge of F127 should be negligible since F127 is
nonionic at the present pH range.
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5
7.
2
1
acid) formed 1D chains in the liquid phase. In this case, the
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