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Top: Illustration of a colloidal nanocrystal
with a cobalt center surrounded by a ligand layer made up of
molecules of an organic surfactant (oleic acid). Bottom: Transmission
electron microscope (TEM) image of cobalt nanocrystals. Scale
bar = 50 nm.
Colloidal nanocrystals have an inorganic core (in this case, cobalt)
surrounded by an organic surfactant, or ligand, layer (in this
case, oleic acid) and are suspended in a liquid solvent (in this
case, 1,2-dichlorobenzene). Cobalt nanocrystals display a wealth
of size-dependent structural, magnetic, electronic, and catalytic
properties. The challenge in making isolated cobalt nanocrystals
is to overcome the large attractive forces between the nanoparticles
due to surface tension and van der Waals interactions that tend
to aggregate them. Using appropriate surfactants, however, cobalt
nanocrystals can be grown with controlled shapes and sizes. It
has been found, for example, that cobalt initially forms disks
in a binary surfactant mixture and that these spontaneously transform
into more thermodynamically stable spheres after heating for a
sufficient period of time. Cobalt nanocrystals with various diameters
can be prepared by simply adjusting the amount of oleic acid used
in the synthesis.
To gain a fundamental understanding of how the properties of nanocrystals
are affected by the growth process, it is necessary to obtain detailed
information of the electronic structure as a function of size and
of the presence and nature of the molecules bound to the surface.
Because cobalt nanocrystals are extremely reactive and oxidize
easily, it is important to use techniques that can interrogate
the particles in their growth environment so that their electronic
and chemical structures can be followed during growth and during
catalytic reactions. Samples of cobalt nanocrystals with diameters
of 3, 4, 5, 6, and 9 nm were grown and suspended in 1,2-dichlorobenzene,
encapsulated in a small liquid cell, and transferred to ALS Beamline
7.0.1 for x-ray spectroscopic experiments.
The most notable feature of the cobalt L-edge XAS spectra is the
new absorption peak, labeled A2, at about 6 eV above the main absorption
edge, A1. This peak is absent in the reference spectra for Co3O4,
CoO, CoCl2, and Co metal. Because the precursors in
the synthesis materials contain only the elements Co, C, O, and
Cl, no other absorption lines are expected near the cobalt L edges.
The researchers believe that this peak is due to a metal-to-ligand
charge transfer (MLCT) transition between the cobalt and the oleic
acid or 1,2-dichlorobenzene. The MLCT satellite peak starts to
appear in nanocrystals of 9 nm and shows an increasing intensity
when the diameter decreases, as expected from the increasing proportion
of cobalt–surfactant molecular interactions.

Left: The most notable feature in the spectra
of the Co nanocrystals (red curves) is the absorption peak (A2)
about 6 eV above the main absorption edge (A1) that is absent
in the reference spectra for Co3O4, CoO,
CoCl2, and Co metal (blue).
Right: Illustration
of MLCT transitions between cobalt and the oleic acid or 1,2-dichlorobezene.
Comparison of the spectra to simulations using the single-impurity
Anderson model showed excellent agreement, and the analysis indicated
that the surface cobalt atoms are aligned in an ordered fashion
to connect the ligands perpendicularly to the nanocrystal surface.
The results also suggested that the nanocrystals interact more
strongly with solvent molecules in the initial stages of growth,
while at a later stage, the interaction is dominated by the oleic
acid surfactant. More generally, experimental and theoretical studies
such as these show that the interaction between cobalt nanocrystals
and surfactant and solvent molecules can be measured by in situ
techniques, opening the way for more detailed studies of growth
and reactivity.
Research conducted by H. Liu, Y. Lin, D.F. Ogletree, and M. Salmeron
(Berkeley Lab); J. Guo (ALS); A. Augustsson (ALS and Uppsala University,
Sweden); C. Dong (ALS and Tamkang University, Taiwan); J. Nordgren
(Uppsala University, Sweden); C. Chang (Tamkang University, Taiwan);
P. Alivisatos (Berkeley Lab and University of California, Berkeley);
G. Thornton (University College London); F.G. Requejo (Universidad
Nacional de La Plata, Argentina); and F. de Groot (Utrecht University,
The Netherlands).
Research funding: U.S. Department of Energy, Office of Basic Energy
Sciences (BES). Operation of the ALS is supported by BES.
Publication about this research: H. Liu, J. Guo, Y. Yin, A. Augustsson,
C. Dong, J. Nordgren, C. Chang, P. Alivisatos, G. Thornton, D.F.
Ogletree, F.G. Requejo, F. de Groot, and M. Salmeron, "Electronic
structure of cobalt nanocrystals suspended in liquid," Nano
Lett. 7, 1919 (2007). |