14 research outputs found
Selective Etching of Copper Sulfide Nanoparticles and Heterostructures through Sulfur Abstraction: Phase Transformations and Optical Properties
Integrating
top-down methods, such as chemical etching, for the
precise removal of excess material in nanostructures with the bottom-up
size and shape control of colloidal nanoparticle synthesis could greatly
expand the range of accessible nanoparticle morphologies. We present
mechanistic insights into an unusual reaction in which trialkylphosphines
(āphosphinesā), which are commonly used to protect nanoparticle surfaces as a surfactant ligand,
chemically etch copper sulfide, Cu<sub>2ā<i>x</i></sub>S, nanostructures in the presence of oxygen. Furthermore, Cu<sub>2ā<i>x</i></sub>S is removed highly selectively
from zinc sulfideīøCu<sub>2ā<i>x</i></sub>S
heterostructures. Structural and optical characterizations show that
the addition of phosphine destabilizes the highly Cu-deficient roxbyite
phase and injects Cu into the interiors of the nanoparticles, even
at room temperature. Analysis of the etching products confirms that
chalcogens are removed in the form of phosphine chalcogenides and
shows that the removed copper is solubilized as Cu<sup>2+</sup>. The
morphology of etched Cu<sub>2ā<i>x</i></sub>S particles
changes dramatically as the concentration of phosphine is reduced,
producing anisotropically etched particles indicative of facet-selective
surface chemical reactions. Additionally, ceric ammonium nitrate,
another oxidizing agent, can be used to control the etching reaction;
the use of this redox agent affords strictly isotropically etched
particles. These results demonstrate the highly pliable structural
and chemical properties of nanocrystalline Cu<sub>2ā<i>x</i></sub>S and raise the possibility of using surface-active
ligands formerly thought to be passivating to dramatically reshape
as-synthesized colloidal nanostructures into more functional forms
Binder-Free and Carbon-Free Nanoparticle Batteries: A Method for Nanoparticle Electrodes without Polymeric Binders or Carbon Black
In this work, we have developed a new fabrication method
for nanoparticle
(NP) assemblies for Li-ion battery electrodes that require no additional
support or conductive materials such as polymeric binders or carbon
black. By eliminating these additives, we are able to improve the
battery capacity/weight ratio. The NP film is formed by using electrophoretic
deposition (EPD) of colloidally synthesized, monodisperse cobalt NPs
that are transformed through the nanoscale Kirkendall effect into
hollow Co<sub>3</sub>O<sub>4</sub>. EPD forms a network of NPs that
are mechanically very robust and electrically connected, enabling
them to act as the Li-ion battery anode. The morphology change through
cycles indicates stable 5ā10 nm NPs form after the first lithiation
remained throughout the cycling process. This NP-film battery made
without binders and conductive additives shows high gravimetric (>830
mAh/g) and volumetric capacities (>2100 mAh/cm<sup>3</sup>) even
after
50 cycles. Because similar films made from drop-casting do not perform
well under equal conditions, EPD is seen as the critical step to create
good contacts between the particles and electrodes resulting in this
significant improvement in battery electrode assembly. This is a promising
system for colloidal nanoparticles and a template for investigating
the mechanism of lithiation and delithiation of NPs
Chalcogenidometallate Clusters as Surface Ligands for PbSe Nanocrystal Field-Effect Transistors
We
introduce a method to process colloidal PbSe nanocrystals (NCs)
into inorganic NC thin films using chalcogenidometallate (ChaM) clusters
as surface ligands, resulting in electrically coupled NC solids. NCs
are first immobilized on a substrate via a self-assembled monolayer
followed by chemical treatment to exchange the insulating oleate ligands
with ChaM clusters. Quantum confinement in the PbSe NCs is preserved
as evidenced by persistent excitonic features in the absorption spectrum.
PbSe NCāChaM composites exhibit rectification (āoffā
states), saturation, n-type electrical behavior, and high electron
mobilities of 1.28 and 0.475 cm<sup>2</sup> V<sup>ā1</sup> s<sup>ā1</sup> for different composite compositions
Reconfigurable Nanorod Films: An <i>in Situ</i> Study of the Relationship between the Tunable Nanorod Orientation and the Optical Properties of Their Self-Assembled Thin Films
Understanding
and controlling the self-assembly of colloidal nanostructures
into ordered superstructures present scientifically interesting and
technologically important research challenges. Here, we investigated
the self-assembly, disordering, and reassembly of colloidal CdSe/CdS
dot/rod nanorod (NR) films. We monitored the structural evolution
of the NR films in real time
using <i>in situ</i> grazing incidence small-angle and wide-angle
X-ray scattering. In dry films, self-assembled from colloidal suspensions,
NRs are oriented with the long axis normal to the substrate, but the
preferred NR orientation is lost when dichlorobenzene vapor is introduced.
Multiprobe optical and structural experiments allowed us to directly
correlate the NR superlattice structure and optical absorption. We
found that the optical absorption of the NR films is significantly
enhanced in disordered NR films compared to NR arrays in which the
rods are oriented normal to the plane of the substrate and parallel
to the optical axis. Basic processingāstructureāproperty
relationships of NR thin films demonstrate that their structure and
optical properties can be reconfigured through the adjustment of solvent
vapor concentration. The phase behavior and optical properties of
NRs present an interesting inorganic analogue to organic liquid crystals
with potential applications in emerging optoelectronic technologies
A Generic Method for Rational Scalable Synthesis of Monodisperse Metal Sulfide Nanocrystals
A rational synthetic method is developed to produce monodisperse
metal sulfide nanocrystals (NCs) in organic nonpolar solutions by
using (NH<sub>4</sub>)<sub>2</sub>S as a sulfide precursor. (NH<sub>4</sub>)<sub>2</sub>S is stabilized in an organic primary amine solution
and exhibits high reactivity toward metal complexes. This novel technique
exhibits wide applicability for organic phase metal sulfide NC synthesis:
a large variety of monodisperse NCs have been synthesized, including
Cu<sub>2</sub>S, CdS, SnS, ZnS, MnS, Ag<sub>2</sub>S, and Bi<sub>2</sub>S<sub>3</sub>. The stoichiometric reactions between (NH<sub>4</sub>)<sub>2</sub>S and metal salts afford high conversion yields, and
large-scale production of monodisperse NCs (more than 30 g) can be
synthesized in a single reaction. The high reactivity of (NH<sub>4</sub>)<sub>2</sub>S enables low temperature (<100 Ā°C) syntheses,
and the air-stable materials (such as CdS NCs) can be produced in
air. Moreover, this low-temperature technique can be used to produce
small size NCs which are difficult to be synthesized by the conventional
high temperature methods, such as sub-5 nm Ag<sub>2</sub>S and Bi<sub>2</sub>S<sub>3</sub> quantum dots
The Oxidation of Cobalt Nanoparticles into Kirkendall-Hollowed CoO and Co<sub>3</sub>O<sub>4</sub>: The Diffusion Mechanisms and Atomic Structural Transformations
We report on the atomic structural
changes and diffusion processes
during the chemical transformation of Īµ-Co nanoparticles (NPs)
through oxidation in air into hollow CoO NPs and then Co<sub>3</sub>O<sub>4</sub> NPs. Through XAS, XRD, TEM, and DFT calculations, the
mechanisms of the transformation from Īµ-Co to CoO to Co<sub>3</sub>O<sub>4</sub> are investigated. Our DFT calculations and experimental
results suggest that a two-step diffusion process is responsible for
the Kirkendall hollowing of Īµ-Co into CoO NPs. The first step
is O in-diffusion by an indirect exchange mechanism through interstitial
O and vacancies of type I Co sites of the Īµ-Co phase. This indirect
exchange mechanism of O has a lower energy barrier than a vacancy-mediated
diffusion of O through type I sites. When the CoO phase is established,
the Co then diffuses outward faster than the O diffuses inward, resulting
in a hollow NP. The lattice orientations during the transformation
show preferential orderings after the single-crystalline Īµ-Co
NPs are transformed to polycrystalline CoO and Co<sub>3</sub>O<sub>4</sub> NPs. Our Co<sub>3</sub>O<sub>4</sub> NPs possess a high ratio
of {110} surface planes, which are known to have favorable catalytic
activity. The Co<sub>3</sub>O<sub>4</sub> NPs can be redispersed in
an organic solvent by adding surfactants, thus rendering a method
to create solution-processable colloidal, monodisperse Co<sub>3</sub>O<sub>4</sub> NPs
Prodigious Effects of Concentration Intensification on Nanoparticle Synthesis: A High-Quality, Scalable Approach
Realizing
the promise of nanoparticle-based technologies demands
more efficient, robust synthesis methods (i.e., process intensification)
that consistently produce large quantities of high-quality nanoparticles
(NPs). We explored NP synthesis via the heat-up method in a regime
of previously unexplored high concentrations near the solubility limit
of the precursors. We discovered that in this highly concentrated
and viscous regime the NP synthesis parameters are less sensitive
to experimental variability and thereby provide a robust, scalable,
and size-focusing NP synthesis. Specifically, we synthesize high-quality
metal sulfide NPs (<7% relative standard deviation for Cu<sub>2ā<i>x</i></sub>S and CdS), and demonstrate a 10ā1000-fold
increase in Cu<sub>2ā<i>x</i></sub>S NP production
(>200 g) relative to the current field of large-scale (0.1ā5
g yields) and laboratory-scale (<0.1 g) efforts. Compared to conventional
synthesis methods (hot injection with dilute precursor concentration)
characterized by rapid growth and low yield, our highly concentrated
NP system supplies remarkably controlled growth rates and a 10-fold
increase in NP volumetric production capacity (86 g/L). The controlled
growth, high yield, and robust nature of highly concentrated solutions
can facilitate large-scale nanomanufacturing of NPs by relaxing the
synthesis requirements to achieve monodisperse products. Mechanistically,
our investigation of the thermal and rheological properties and growth
rates reveals that this high concentration regime has reduced mass
diffusion (a 5-fold increase in solution viscosity), is stable to
thermal perturbations (ā¼64% increase in heat capacity), and
is resistant to Ostwald ripening
Highly Conductive Cu<sub>2ā<i>x</i></sub>S Nanoparticle Films through Room-Temperature Processing and an Order of Magnitude Enhancement of Conductivity via Electrophoretic Deposition
A facile room-temperature method
for assembling colloidal copper sulfide (Cu<sub>2ā<i>x</i></sub>S) nanoparticles into highly electrically conducting films
is presented. Ammonium sulfide is utilized for connecting the nanoparticles
via ligand removal, which transforms the as-deposited insulating films
into highly conducting films. Electronic properties of the treated
films are characterized with a combination of Hall effect measurements,
field-effect transistor measurements, temperature-dependent conductivity
measurements, and capacitanceāvoltage measurements, revealing
their highly doped p-type semiconducting nature. The spin-cast nanoparticle
films have carrier concentration of ā¼10<sup>19</sup> cm<sup>ā3</sup>, Hall mobilities of ā¼3 to 4 cm<sup>2</sup> V<sup>ā1</sup> s<sup>ā1</sup>, and electrical conductivities
of ā¼5 to 6 SĀ·cm<sup>ā1</sup>. Our films have hole
mobilities that are 1ā4 orders of magnitude higher than hole
mobilities previously reported for heat-treated nanoparticle films
of HgTe, InSb, PbS, PbTe, and PbSe. We show that electrophoretic deposition
(EPD) as a method for nanoparticle film assembly leads to an order
of magnitude enhancement in film conductivity (ā¼75 SĀ·cm<sup>ā1</sup>) over conventional spin-casting, creating copper
sulfide nanoparticle films with conductivities comparable to bulk
films formed through physical deposition methods. The X-ray diffraction
patterns of the Cu<sub>2ā<i>x</i></sub>S films, with
and without ligand removal, match the Djurleite phase (Cu<sub>1.94</sub>S) of copper sulfide and show that the nanoparticles maintain finite
size after the ammonium sulfide processing. The high conductivities
reported are attributed to better interparticle coupling through the
ammonium sulfide treatment. This approach presents a scalable room-temperature
route for fabricating highly conducting nanoparticle assemblies for
large-area electronic and optoelectronic applications
Synthesis and Properties of Electrically Conductive, Ductile, Extremely Long (ā¼50 Ī¼m) Nanosheets of K<sub><i>x</i></sub>CoO<sub>2</sub>Ā·<i>y</i>H<sub>2</sub>O
Extremely long, electrically conductive,
ductile, free-standing
nanosheets of water-stabilized K<sub><i>x</i></sub>CoO<sub>2</sub>Ā·<i>y</i>H<sub>2</sub>O are synthesized using
the solāgel and electric-field induced kinetic-demixing (SGKD)
process. Room temperature in-plane resistivity of the K<sub><i>x</i></sub>CoO<sub>2</sub>Ā·<i>y</i>H<sub>2</sub>O nanosheets is less than ā¼4.7 mĪ©Ā·cm, which corresponds
to one of the lowest resistivity values reported for metal oxide nanosheets.
The synthesis produces tens of thousands of very high aspect ratio
(50,000:50,000:1 = length/width/thickness), millimeter length nanosheets
stacked into a macro-scale pellet. Free-standing nanosheets up to
ā¼50 Ī¼m long are readily delaminated from the stacked
nanosheets. High-resolution transmission electron microscopy (HR-TEM)
studies of the free-standing nanosheets indicate that the delaminated
pieces consist of individual nanosheet crystals that are turbostratically
stacked. X-ray diffraction (XRD) studies confirm that the nanosheets
are stacked in perfect registry along their <i>c</i>-axis.
Scanning electron microscopy (SEM) based statistical analysis show
that the average thickness of the nanosheets is ā¼13 nm. The
nanosheets show ductility with a bending radius as small as ā¼5
nm
Direct Measurements of Surface Scattering in Si Nanosheets Using a Microscale Phonon Spectrometer: Implications for Casimir-Limit Predicted by Ziman Theory
Thermal
transport in nanostructures is strongly affected by phonon-surface
interactions, which are expected to depend on the phononās
wavelength and the surface roughness. Here we fabricate silicon nanosheets,
measure their surface roughness (ā¼1 nm) using atomic force
microscopy (AFM), and assess the phonon scattering rate in the sheets
with a novel technique: a microscale phonon spectrometer. The spectrometer
employs superconducting tunnel junctions (STJs) to produce and detect
controllable nonthermal distributions of phonons from ā¼90 to
ā¼870 GHz. This technique offers spectral resolution nearly
10 times better than a thermal conductance measurement. We compare
measured phonon transmission rates to rates predicted by a Monte Carlo
model of phonon trajectories, assuming that these trajectories are
dominated by phonon-surface interactions and using the Ziman theory
to predict phonon-surface scattering rates based on surface topology.
Whereas theory predicts a diffuse surface scattering probability
of less than 40%, our measurements are consistent with a 100% probability.
Our nanosheets therefore exhibit the so-called āCasimir limitā
at a much lower frequency than expected if the phonon scattering rates
follow the Ziman theory for a 1 nm surface roughness. Such a result
holds implications for thermal management in nanoscale electronics
and the design of nanostructured thermoelectrics