A long-standing goal for the preparation of nano-scale materials
is the development of a general synthetic methodology that allows
low temperature, solution phase growth methods, that yields
crystalline materials. We have generalized a strategy that utilizes
inorganic clusters as single source precursors for the preparation
of II-VI nanocrystals between the sizes of 2-10 nm, including
CdSe, ZnSe, CdS, and ZnS. (Figure 1) The use of a cluster based
single source precursor allows nanocrystal growth to be initiated
without a requisite pyrolytic step for nucleus formation, which
is traditionally required for lyothermal growth mechanisms.
The elimination of the pyrolytic step allows greater synthetic
control, slow thermodynamic growth at lower temperatures, and
large scale reactions (> 50 g/L) to be prepared, while maintaining
size-dispersity at < 5% and crystallinity. We have continued
to explore the properties of nanocrystal growth using inorganic
clusters as single source precursors, extending the methodology
to Co metal nanoparticles, III-V nanocrystals, and doped nanocrystals.
We have extended our crystal seeding methodology, which employs
the introduction of a preformed metal-chalcogenide cluster to
a coordinating solvent to CdSe, CdSe, ZnSe, ZnS, and CdSe/ZnS
(Core/shell materials). The use of a [M10Se4SPh16]4- cluster
as the preformed nucleus in a long-chain alkyl amine, hexadecylamine
for example, allows growth of crystalline nanocrystals (5% rms
batch, <4% rms selectively precipitated) (Figure 2). Owing
to the rapid ligand and metal exchange in these materials, nucleation
occurs instantly at relatively low temperatures followed by
growth of the nanocrystals under thermal control. The reaction
mechanism is believed to proceed via a step wise nucleation
and growth via addition of a second cluster to an initial nucleus.
The size of the nanomaterial can be tuned by solvent temperature
in this reaction. It appears this may arise from the fact the
surface energy of these structures allow rapid rearrangement
with formation of the lowest energy nanocrystal, suggesting
controlled thermodynamic growth can be achieved in these materials.
Uniquely, the preparative route using an inorganic seeds results
in a narrow size distributuion without the observation of small
nanocrystals in the reaction mixture. This methodology allows
preparation of large scale reactions of organically passivated,
spherical nanocrystals (> 50g/L) of CdSe and ZnSe (2-10 nm,
<5% rms size selectively precipitated, 5% thermally annealed
or 6-12% out of batch). The CdSe can be recapped with an inorganic
passivant layer (ZnS) following traditional lyothermal techniques
to yield CdSe/ZnS core-shell structures. A major advantage of
this new methodology is the attainment of greater synthetic
control.
Interested in learning more?
Contact Dr. Strouse
or
read the published article:
"Inorganic Clusters as Single
Source Precursors for Preparation of CdSe, ZnSe, CdSe/ZnS
Nanomaterials." Cumberland, S.L.; Hanif, K.M.;
Javier, A.; Khitrov, G.A.; Strouse, G.F.; Woessner, S.M.;
Yun, C.S. Chem. Mater.,
14, 1576-1584 (2002). [ view
article - PDF ]

Doping bulk semiconductors with metal ions, for example Mn(II),
Co(II), Eu(II), Cu(II), or V(II), has been demonstrated to significantly
tune the observed optical and magnetic properties in the new
ternary complex. Interstitial doping has been shown to lead
to cooperative effects between the semiconductor host lattice
and transition metal guest ions arising from long range exchange
interactions. The influence on the physical properties is proportional
to the doping level, and material choice. Recent studies on
doping nano-scale materials have suggested doping is poorly
achieved in materials on the nanoscale due primarily to lattice
annealing during lyothermal growth, which tends to lead to surface
doping of the materials. Development of new methods for the
preparation of quantum dot semiconductor structures doped with
transition metal ions could provide a rich opportunity to explore
the relationship between structure and transport properties
on varying length scales in reduced dimensions.
Systematic core doping of CdSe between 0 and 40% with a selected
dopant has been achieved by treatment with appropriately doped
precursors. Several manuscripts on this effort will be submitted
later this year outlining the results of doping with V, Cu,
Co, and Eu dopants (2 of which are currently in preparation).
The emphasis of this effort targets the preparation of discrete
II-VI nano-crystalline materials doped both interstitially and
at the surface with transition metal ions to induce magnetic
coupling between quantum dots. Using a novel single source precursor
route, our group has prepared a series of transition metal (Co,
Cu, V) and lanthanide (Eu) doped CdSe nanoparticles that exhibit
a narrow size dispersity (2-8 nm diameter, 5% relative standard
deviation of size). The strategy for doping is analogous to
the single source precursor method above with the modification
of either the addition of an inorganic salt (Eu, V) to the initial
reaction mixture, or the addition of an inorganic cluster (Co,
Cu). Analysis of the AA, ICP-AES, TEM-EDX and atomic absorption
confirm the Cd1-xMxSe (M= Cu, Co, Eu, V) materials are doped
in the core at levels between x = 0.00 and 0.4.
Corroborating the core-level doping, these materials exhibit
a linear shift in the powder X-ray diffraction with doping concentration,
in analogy to shifts observed in doped bulk materials. The linear
shift in the X-ray parameters is consistent with core-level
doping, and provides the first reported evidence of controlled
core-doping in II-VI materials. The lattice shift can be understood
in terms of a solid-state approximation, in which a similar
shift in lattice parameters is observed for statistical doping
of the cores of the materials, rather than surface doping (Vegards
Law). Furthermore, extrapolation of the M-Se bond distances
to a lattice composed of 100% EuSe or CoSe produce a M-Se bond
distance consistent with the bonding in pure materials.
Magnetic and optical studies on Co(II) doped CdSe provide further
evidence for controlled doping. In the Co(II) doped materials
a signature for a Co centered longitudinal optical phonon is
evident at ~ 300 cm-1 and scales with Co concentration further
corroborating core-level doping in these materials. Recent XPS
and EXAFS results suggest the Co may be doped as Co-O, possibly
due to core vs surface level doping. Magnetic studies indicate
the onset of spin glass behavior below the bulk percolation
threshold in these materials, which suggest enhanced quantum
confinement may lead to extended magnetic coupling in these
materials. Analysis of the magnetic coupling as a function of
nanomaterial size and composition is providing unique insight
into the structure, and magnetic properties of materials in
the quantum confined limit.
Interested
in learning more?
Contact Dr. Strouse
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