C O M M U N I C A T I O N S
Figure 3. (a) A typical HRTEM image of a selected area of an individual
Ag nanocube with the SAED pattern shown in the inset. (b) The nanocube
used for the HRTEM and SAED studies with the area marked with a white
pane indicating where the HRTEM image was recorded. (c) Schematic
illustration of the facets of an individual cube.
Figure 4. (a-d) TEM images of Ag NPs synthesized with various molar
ratios of HTAB/[Ag(NH3)2]+: (a) 1, (b) 1.5, (c) 2.5, (d) 3. (e, f) photos
and UV/vis absorption spectra of the aqueous solutions of the Ag NPs,
marked with 1, 2, 3, and 4 corresponding to those of the Ag NPs shown in
panels a, b, c, and d, respectively.
are ca. 5 nm. Such a regular assembly of the cubes is due to the
facts that the HTAB adsorbed on the cube surfaces would form a
capping shell to generate a regular interparticle spacing and thus
to prevent the cubes from random aggregation,12 and that the
uniformity of the sample made it possible to manipulate the cubes
into a close-packed and ordered array caused by van der Waals
forces.13
In summary, monodisperse silver nanocubes with edge length
of 55 ( 5 nm were, for the first time, synthesized in water on the
basis of HTAB-modified silver mirror reaction. Their high stability
in water would be favorable for further chemical modification and
systematic investigations. Their 2D array with regular checked
pattern on solid substrate may open up the possibilities of fabricating
new nanodevices with novel physical properties, because the
coupling between proximal NPs may give rise to new collective
phenomena. Considering the unique properties of silver, its
nanocubes should be of importance for both theoretical investiga-
tions and practical applications.
Figure 3a shows the high-resolution TEM (HRTEM) image of
a cube as indicated in Figure 3b. The inset shows the corresponding
selected area electron diffraction (SAED) pattern, obtained by
directing the incident electron beam perpendicular to one of the
square facets of the cube. The square spot array was indexed to
[200] and [020] of the fcc silver. The 2D lattice fringes of the
HRTEM image were examined to be 0.204 nm, close to the {200}
lattice spacing of the fcc silver. Because the HRTEM image was
recorded from the area along one upright facet as marked by a
white pane in Figure 3b, the perpendicular fringes were either
parallel to or orthogonal to the upright facet of the cube, suggesting
that the six surfaces of the silver nanocubes consisted of {200}
lattice planes as schematically illustrated in Figure 3c. Note that
our HRTEM images clearly showed that the edges of the cubes
were not bounded by {110} as described by Xia,6 but actually they
consisted of small bent faces. On the basis of the TEM and HRTEM
analyses, it could be concluded that when these regular nanocubes
bounded by {200} facets assembled into a 2D array on a substrate,
they, of course, had an identical [001] zone direction, thus resulting
in the strongest diffraction of (200) as shown in the XRD pattern.
As an ionic surfactant, HTAB played multiple roles in the
formation of the nanocubes. It acted not only as the reaction
moderator as described above but also as the shape controller and
stabilizing agent. First of all, its micelles directed the silver metal
to nucleate and grow into NPs other than the usual silver mirror.
As shown in Figure 4a-d, an increase in the molar ratio of HTAB/
[Ag(NH3)2]+ led to an obvious shape evolution of silver NPs from
spheres to cubes, which was caused by the anisotropic adsorption
of the surfactant on the silver crystal faces, while such adsorption
characteristics depended on the molar ratio.14 When the molar ratio
reached ca. 1.5, anisotropic growth of the particles appeared as
indicated by the arrows in Figure 4b. When the molar ratio increased
further to 2.5, the product was dominated by nanocubes (Figure
4c). Second, it stabilized the silver NPs to form stable aqueous
solutions (Figure 4e), the color of which changed from orange to
yellow with the increase of the molar ratio. Note that the nanocubes
also showed an absorption band at ca. 420 nm (Figure 4f, curve
4), typical of the plasmon resonance of the spherical silver NPs,
since the nanocubes assumed bent edges rather than sharp ones
such as triangles or prisms.2a More detailed investigation on their
optical properties is still in progress.
Acknowledgment. V.W.-W.Y. acknowledges the financial
support from the University Development Fund (UDF) of The
University of Hong Kong and The University of Hong Kong
Foundation for Educational Development and Research Limited.
Supporting Information Available: Preparation and characteriza-
tion, calculation of the equilibrium constant, EDX spectrum, HRTEM
image and analysis. This material is available free of charge via the
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