C O M M U N I C A T I O N S
solution conditions of this complex mixture of diluted bicellar
2
,18,19
solution, Pt salt and aqueous AA, and the different pH (2.7).
In this mixture, the hydrodynamic size could also be increased by
bicellar aggregation and the presence of other mesophases. Nev-
ertheless, a bicellar diameter of 602 nm calculated from the
hydrodynamic diameter (details given in the Supporting Informa-
tion) is compatible with the diameter of the Pt nanowheels obtained
from electron microscopy (496 nm), especially given that Pt sheet
growth might shrink the bicelles.
To conclusively demonstrate that the flaring at the edge of the
Pt nanowheels is a consequence of nanosheet growth reaching the
edge of the bicelle, we lowered the Pt(II) concentration from 10 to
5
mM while holding the other parameters constant. For this case,
circular dendritic nanodisks with thickened centers are observed,
but without the flaring (Figures 3b and S6a). This was expected
because the Pt complex is consumed before the sheet reaches the
edge of the bicelle. This also provides further proof that the
nanowheel grows outward from a central nucleation site.
Figure 3. (a) DLS size distributions of bicelles in stock suspension
containing 1 mM of CTAB and FC7 (blue), and three repetions for the
reaction system containing bicelles, Pt(II) salt, and AA (0.5 mM CTAB
and FC7, 10 mM K2PtCl4, and 150 mM AA (red)). (b) TEM image of
platinum nanodisks.
Finally, when the original synthesis was conducted at 30 and 20
C, nanowheels with small and large flarings at the edges (Figure
are thickened (Figure 2a). The central thickening is possibly due to
the fact that dendritic growth is initiated at a centrally located seed
nanoparticle. Slow growth normal to the surface of the sheet occurs
throughout the reduction reaction and is thus most extensive near the
center of the sheet where growth occurs for the longest time. The reason
that the seed particles locate at the center of the bicelle may be due to
°
S6b,c) were observed, respectively. This is consistent with the
production of fewer bicelles containing seed particles at low
temperature, leaving more Pt complex per seed and thus more
extensive growth for the fewer seeded bicelles. Variation of total
surfactant concentration provides additional opportunities to direct
the growth of Pt to produce complex nanostructures. The metal
growth methods described here might also be used as a means of
imaging and discovering structural features of other types of
surfactant assemblies and other templating materials.
4
electrostatic forces caused by the high positive charge density at the
edge of the bicelles. A radial mechanical stress also likely exists in
the bicelle because the layers are bound together more tightly at the
highly curved edge than at the loose central region, which can thus
more easily accommodate the Pt seed particle.
The high-angle annular dark-field scanning TEM (HAADF
STEM) images (Figure 2b), for which the brightness is related to
the Pt density, confirm that the rim and the center are much more
dense than the intermediate region. Additionally, the Pt density
profile (Figure 2, inset) indicates that the disk-like part between
the center and the edge is roughly uniform in thickness. Consistent
with other dendritic Pt sheets formed in lipid bilayers, the thickness
is estimated to be about 2 nm. This can be seen by comparing
the size of dendritic tips and the width of bright lines originating
from the approximately vertically aligned dendritic branches in the
edge region (see Figure S4). In high-magnification images (Figure
Acknowledgment. Sandia is a multiprogram laboratory operated
by Sandia Corporation, a Lockheed Martin Company, for the U.S.
Department of Energy’s National Nuclear Security Administration
under Contract DEAC04-94AL85000.
Supporting Information Available: Experimental details; UV-vis
spectrum; SEM, TEM, and STEM images; size analysis plot; and XRD
pattern. This material is available free of charge via the Internet at
http://pubs.acs.org.
1
3
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