3 research outputs found
Correlating Carrier Density and Emergent Plasmonic Features in Cu<sub>2–<i>x</i></sub>Se Nanoparticles
Recently, a wide variety of new nanoparticle
compositions have been identified as potential plasmonic materials
including earth-abundant metals such as aluminum, highly doped semiconductors,
as well as metal pnictides. For semiconductor compositions, plasmonic
properties may be tuned not only by nanoparticle size and shape, but
also by charge carrier density which can be controlled via a variety
of intrinsic and extrinsic doping strategies. Current methods to quantitatively
determine charge carrier density primarily rely on interpretation
of the nanoparticle extinction spectrum. However, interpretation of
nanoparticle extinction spectra can be convoluted by factors such
as particle ligands, size distribution and/or aggregation state which
may impact the charge carrier information extracted. Therefore, alternative
methods to quantify charge carrier density may be transformational
in the development of these new materials and would facilitate previously
inaccessible correlations between particle synthetic routes, crystallographic
features, and emergent optoelectronic properties. Here, we report
the use of <sup>77</sup>Se solid state nuclear magnetic resonance
(NMR) spectroscopy to quantitatively determine charge carrier density
in a variety of Cu<sub>2–<i>x</i></sub>Se nanoparticle
compositions and correlate this charge carrier density with particle
crystallinity and extinction features. Importantly, we show that significant
charge carrier populations are present even in nanoparticles without
spectroscopically discernible plasmonic features and with crystal
structures indistinguishable from fully reduced Cu<sub>2</sub>Se.
These results highlight the potential impact of the NMR-based carrier
density measurement, especially in the study of plasmon emergence
in these systems (i.e., at low dopant concentrations)
Efficient Energy Transfer from Near-Infrared Emitting Gold Nanoparticles to Pendant Ytterbium(III)
Here,
we demonstrate efficient energy transfer from near-infrared-emitting <i>ortho</i>-mercaptobenzoic acid-capped gold nanoparticles (AuNPs)
to pendant ytterbiumÂ(III) cations. These functional materials combine
the high molar absorptivity (1.21 × 10<sup>6</sup> M<sup>–1</sup> cm<sup>–1</sup>) and broad excitation features (throughout
the UV and visible regions) of AuNPs with the narrow emissive properties
of lanthanides. Interaction between the AuNP ligand shell and ytterbium
is determined using both nuclear magnetic resonance and electron microscopy
measurements. In order to identify the mechanism of this energy transfer
process, the distance of the ytterbiumÂ(III) from the surface of the
AuNPs is systematically modulated by changing the size of the ligand
appended to the AuNP. By studying the energy transfer efficiency from
the various AuNP conjugates to pendant ytterbiumÂ(III) cations, a Dexter-type
energy transfer mechanism is suggested, which is an important consideration
for applications ranging from catalysis to energy harvesting. Taken
together, these experiments lay a foundation for the incorporation
of emissive AuNPs in energy transfer systems
Clathrate Ba<sub>8</sub>Au<sub>16</sub>P<sub>30</sub>: The “Gold Standard” for Lattice Thermal Conductivity
A novel clathrate phase, Ba<sub>8</sub>Au<sub>16</sub>P<sub>30</sub>, was synthesized from its elements.
High-resolution powder X-ray
diffraction and transmission electron microscopy were used to establish
the crystal structure of the new compound. Ba<sub>8</sub>Au<sub>16</sub>P<sub>30</sub> crystallizes in an orthorhombic superstructure of
clathrate-I featuring a complete separation of gold and phosphorus
atoms over different crystallographic positions, similar to the Cu-containing
analogue, Ba<sub>8</sub>Cu<sub>16</sub>P<sub>30</sub>. Barium cations
are trapped inside the large polyhedral cages of the gold–phosphorus
tetrahedral framework. X-ray diffraction indicated that one out of
15 crystallographically independent phosphorus atoms appears to be
three-coordinate. Probing the local structure and chemical bonding
of phosphorus atoms with <sup>31</sup>P solid-state NMR spectroscopy
confirmed the three-coordinate nature of one of the phosphorus atomic
positions. High-resolution high-angle annular dark-field scanning
transmission electron microscopy indicated that the clathrate Ba<sub>8</sub>Au<sub>16</sub>P<sub>30</sub> is well-ordered on the atomic
scale, although numerous twinning and intergrowth defects as well
as antiphase boundaries were detected. The presence of such defects
results in the pseudo-body-centered-cubic diffraction patterns observed
in single-crystal X-ray diffraction experiments. NMR and resistivity
characterization of Ba<sub>8</sub>Au<sub>16</sub>P<sub>30</sub> indicated
paramagnetic metallic properties with a room-temperature resistivity
of 1.7 mΩ cm. Ba<sub>8</sub>Au<sub>16</sub>P<sub>30</sub> exhibits
a low total thermal conductivity (0.62 W m<sup>–1</sup> K<sup>–1</sup>) and an unprecedentedly low lattice thermal conductivity
(0.18 W m<sup>–1</sup> K<sup>–1</sup>) at room temperature.
The values of the thermal conductivity for Ba<sub>8</sub>Au<sub>16</sub>P<sub>30</sub> are significantly lower than the typical values reported
for solid crystalline compounds. We attribute such low thermal conductivity
values to the presence of a large number of heavy atoms (Au) in the
framework and the formation of multiple twinning interfaces and antiphase
defects, which are effective scatterers of heat-carrying phonons