NATURE NANOTECHNOLOGY | VOL 5 | JANUARY 2010 | www.nature.com/naturenanotechnology 15
REVIEW ARTICLE
PUBLISHED ONLINE: 24 DECEMBER 2009 | DOI: 10.1038/NNANO.2009.453
C
urrent interest in ensembles of inorganic nanoparticles is
motivated by our ability to exploit their collective properties and
the possibility of using these properties in functional devices.
Ensembles of nanoparticles can be used to improve the mechanical
properties of composite materials, and they can also allow multiple
tasks to be performed simultaneously or in sequence. Ensembles of
nanoparticles can also display new electronic, magnetic and optical
properties as a result of interactions between the excitons, magnetic
moments or surface plasmons of individual nanoparticles. It should
be possible to exploit these properties in devices, and also the direc-
tionality and long-range order found in ensembles, if the spacing and
alignment of individual nanoparticles can be controlled.
Self-assembly provides a simple and low-cost method for pro-
ducing ensembles of nanoparticles in a controllable manner, and
in this review we summarize recent advances in the ield. We start
with a summary of various methods for the self-assembly or assisted
assembly of nanoparticles (see refs 1–6 for more detailed reviews),
and then go on to review the properties of self-assembled nano-
particle structures and possible applications for these structures. We
restrict ourselves to systems in which the distance between nano-
particles is comparable to the nanoparticle size and do not, therefore,
discuss nanoparticle patterning or alignment, or the self-assembly of
secondary nanoparticle structures (such as nanowires), unless these
methods are used to create close-packed structures.
Strategies for self-assembly of nanoparticles
Self-assembly in solution. Figure 1 illustrates the self-assembly of
nanoparticles in solutions in the absence of templates, interfaces or
external ields. Assembly is governed by the balance of attractive
forces (such as covalent or hydrogen bonding, electrostatic attraction
between oppositely charged ligands, depletion forces or dipole–dipole
interactions) and repulsive forces (such as steric forces and electro-
static repulsion between ligands of like charge)
7
. Self-organization of
nanoparticles generates a variety of structures, including chains
8–11
,
sheets
12,13
, vesicles
9,14,15
, three-dimensional (3D) crystals
16–19
or more
complex 3D architectures
20
.
One approach to solution-based self-assembly exploits site-spe-
ciic interactions of chemically heterogeneous nanoparticles
9,21
. For
Properties and emerging applications of
self-assembled structures made from inorganic
nanoparticles
Zhihong Nie
1†
, Alla Petukhova
1†
and Eugenia Kumacheva
1,2,3
*
Just as nanoparticles display properties that difer from those of bulk samples of the same material, ensembles of nanoparticles
can have collective properties that are diferent to those displayed by individual nanoparticles and bulk samples. Self-assembly
has emerged as a powerful technique for controlling the structure and properties of ensembles of inorganic nanoparticles. Here
we review diferent strategies for nanoparticle self-assembly, the properties of self-assembled structures of nanoparticles, and
potential applications of such structures. Many of these properties and possible applications rely on our ability to control the
interactions between the electronic, magnetic and optical properties of the individual nanoparticles.
example, end-by-end or side-by-side assembly of gold nanorods
can be driven by triggering attraction between the distinct ligands
attached to the long and short facets of the nanorod
9
. Figure 1b shows
assemblies of gold nanorods carrying cetyl trimethyl ammonium bro-
mide (CTAB) on the long nanorod side and polystyrene molecules at
the nanorod ends. his method used the analogy between the nano-
rods and ABA triblock copolymers
9,22,23
: the addition of water (a bad
solvent for polystyrene) to a solution of nanorods in dimethyl forma-
mide produced nanorod chains, whereas the addition of water to a
solution of nanorods in tetrahydrofurane (a bad solvent for CTAB)
triggered nanorod assembly in bundles.
Chemical heterogeneity of nanoparticles was also induced by
phase separation between ‘immiscible’ organic ligands
8,24
or consecu-
tive attachment of diferent ligands
21,25
. Phase separation in a mixture
of nonanoic acid and 4-phenylbutyric acid produced two distinct sin-
gularities on the surface of γ-Fe
2
O
3
nanoparticles, which allowed for
the subsequent reaction with the molecular linker and the formation
of nanoparticle chains (Fig. 1c)
24
.
Alternatively, a balance of the anisotropic hydrophobic attraction
and electrostatic interactions (originating from a dipole moment and
a small positive charge of nanoparticles) governed the spontaneous
formation of close-packed monolayer sheets of CdTe nanoparticles
coated with 2-(dimethylamino)ethanethiol (Fig. 1d)
12
. he experi-
mental results were supported by computer simulations of interpar-
ticle interactions.
Recently, the formation of 3D nanoparticle crystals with
face-centred or body-centred cubic lattice structures was mediated
by hybridizing complementary DNA molecules attached to the nano-
particle surface
17,18
. he variation in DNA sequences or length of DNA
linkers, and the absence or presence of a non-bonding single-base
lexor, was used to tune interactions between the nanoparticle–DNA
conjugates. Figure 1e shows a fragment of the crystal with the body-
centred cubic structure formed by gold nanoparticles
17
. In a difer-
ent strategy, crystals with a diamond-like structure were grown from
oppositely charged gold and silver nanoparticles
16
. Crystallization of
nanoparticles was achieved by screening electrostatic interactions, so
that each nanoparticle was surrounded by a layer of counter-ions and
the nanoparticles interacted by short-range potentials.
1
Department of Chemistry, University of Toronto, 80 Saint George Street, Toronto, Ontario M5S 3H6, Canada,
2
Department of Chemical Engineering
and Applied Chemistry, University of Toronto, 200 College Street, Toronto, Ontario M5S 3E5, Canada,
3
Institute of Biomaterials and Biomedical Engineering
University of Toronto, 4 Taddle Creek Road, Toronto, Ontario M5S 3G9, Canada.
†
These authors contributed equally to this article.
*e-mail: ekumache@chem.utoronto.ca
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