RSC Advances
Paper
2.8 to 12 nm were obtained by simply control the reaction time.
Cubic berzelianite crystal phase and narrow size distributions
were demonstrated by the characterization results. The cubic
berzelianite phase and chemical compositions for Cu/Se of
1.6 : 1 were demonstrated. With the assistance of OAM, as-
synthesized narrow size distributed Cu2ꢀxSe nanocrystals self-
assembled into ordered superstructures.
Fig. 4 (A)–(C) TEM images and corresponding FFT patterns of trian-
gular Cu2ꢀxSe nanocrystals with different assemble behaviors; inset:
corresponding Schemes of the stacking of triangular Cu2ꢀxSe
nanocrystals.
Acknowledgements
This work was nancially supported by the research project of
the National Natural Science Foundation of China (21201055),
Natural Science Research Program of Henan Educational
Committee, China (12A430003), and Doctoral Foundation of
Henan Institute of Engineering (D2012019 and D2010011).
in the spectrum which indicated the presence of +2 valence
state in the Cu2ꢀxSe nanocrystals. All that suggesting that the
copper valence state in the Cu2ꢀxSe nanocrystals is compound
of +1 and +2. Fig. 3D shows the Se 3d5/2 peak located at 52.5 eV,
References
indicating Se2ꢀ
.
It is well known that monodisperse triangular nanocrystals
are ideal building blocks for novel two-dimensional (2D)
superlattices. In our experiments, the evaporation of carrier
solvent of the nanocrystals led triangular Cu2Se nanocrystals to
self-assemble into superlattices as shown in Fig. 4. The corre-
sponding fast Fourier transformation (FFT) of these three
images conrms the well-ordered structures with different
tendency and also reveals the close-packing of Cu2ꢀxSe nano-
crystals. There are two reasons for the triangle-shaped Cu2ꢀxSe
nanocrystals can self-assemble into two-dimensional super-
lattice on the TEM grid: rst, the narrow size distributions of
Cu2ꢀxSe nanocrystals. In a nanocrystal superlattice, the indi-
vidual nanocrystals with nearly same size act as atoms in a
crystal lattice. The attraction and repulsion between neighbour
particles are size dependent,31 nearly same size means that the
interaction forces could be well balanced with same distance
between particles and ordered structures could be formed.
While, without narrow size distribution, ordered structures are
hard to form, as indicated by Fig. 1A–C. Second, the OAM
molecules on the nanocrystal surface. The van der Waals
interactions which arise from the long alkyl chain of OAM
molecules capping on the surface of the nanocrystals provides
the attractive force to induce the self-assembly. And more, the
presence of OAM in the solvent mixture provides a lasting
wetting layer for nanocrystals to diffuse to their equilibrium
sites by the entropy driven ordering tendency.32 Molecular
dynamics simulations done by Luedtke and Landman have
shown that organic capping ligands (such as OAM) can lubri-
cate the interface, giving nanocrystals a high surface mobility
and play critical roles in reducing the activity of nanocrystals
(building blocks) to promote or tune the ordered self-
assembly.33,34
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39550 | RSC Adv., 2014, 4, 39547–39551
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