15 research outputs found
Functional Monolithic Polymeric Organic Framework Aerogel as Reducing and Hosting Media for Ag nanoparticles and Application in Capturing of Iodine Vapors
Monolithic aerogels of polymeric organic framework (Mon-POF)
with
a high density of OH functional groups were synthesized through solvothermal
polymerization of terephthalaldehyde and 1,5-dihydroxynaphthalene.
This POF material presents high surface area of 1230 m<sup>2</sup> g<sup>–1</sup> having micro-, meso-, macropores, and low
bulk density of 0.15 g cm<sup>–3</sup>. The evolution of the
porous properties is controlled with the polymerization rate. Mon-POF
is stable under acidic and basic conditions. The presence of high
number of OH functional groups provides the monolith with ion-exchange
properties as well as reducing properties. The Mon-POF adsorbs Ag<sup>+</sup> from aqueous solution to deposit Ag nanoparticles into the
pores at a high loading content ∼25 wt % of the composite material.
The Ag loaded monolith captures significant amount of I<sub>2</sub> vapor and fixes it effectively in the form of β-AgI
Selective Surfaces: Quaternary Co(Ni)MoS-Based Chalcogels with Divalent (Pb<sup>2+</sup>, Cd<sup>2+</sup>, Pd<sup>2+</sup>) and Trivalent (Cr<sup>3+</sup>, Bi<sup>3+</sup>) Metals for Gas Separation
Porous chalcogels with tunable compositions of Co<sub><i>x</i></sub>M<sub>1<i>–x</i></sub>MoS<sub>4</sub> and
Ni<sub><i>x</i></sub>M<sub>1–<i>x</i></sub>MoS<sub>4</sub>, where M = Pd<sup>2+</sup>, Pb<sup>2+</sup>, Cd<sup>2+</sup>, Bi<sup>3+</sup>, or Cr<sup>3+</sup> and <i>x</i> = 0.3–0.7, were synthesized by metathesis reactions between
the metal ions and MoS<sub>4</sub><sup>2–</sup>. Solvent exchange,
counterion removal and CO<sub>2</sub> supercritical drying led to
the formation of aerogels. All chalcogels exhibited high surface areas
(170–510 m<sup>2</sup>/g) and pore volumes in the 0.56–1.50
cm<sup>3</sup>/g range. Electron microscopy coupled with nitrogen
adsorption measurements suggest the presence of both mesoporosity
(2 nm < <i>d</i> < 50 nm) and macroporosity (<i>d</i> > 50 nm, where <i>d</i> is the average pore
size). Pyridine adsorption corroborated for the acid character of
the aerogels. We present X-ray photoelectron spectroscopic and X-ray
scattering evidence that the [MoS<sub>4</sub>]<sup>2–</sup> unit does not stay intact when bound to the metals in the chalcogel
structure. The Mo<sup>6+</sup> species undergoes redox reactions during
network assembly, giving rise to Mo<sup>4+/5+</sup>-containing species
where the Mo is bound to sulfide and polysulfide ligands. The chalcogels
exhibit high adsorption selectivities for CO<sub>2</sub> and C<sub>2</sub>H<sub>6</sub> over H<sub>2</sub>, N<sub>2</sub>, and CH<sub>4</sub> whereas specific compositions exhibited among the highest
CO<sub>2</sub> enthalpy of adsorption reported so far for a porous
material (up to 47 kJ/mol). The Co-Pb-MoS<sub>4</sub> and Co-Cr-MoS<sub>4</sub> chalcogels exhibited a 2-fold to 4-fold increase in CO<sub>2</sub>/H<sub>2</sub> selectivity compared to ternary CoMoS<sub>4</sub> chalcogels
Seeing Is Believing: Weak Phonon Scattering from Nanostructures in Alkali Metal-Doped Lead Telluride
Alkali metal doped p-type PbTe is a canonical thermoelectric
material
studied extensively for heat-to-power generation at high temperature.
Most reports have indirectly indicated alkali metals to be conventional
with PbTe forming homogeneous solid solutions. Using transmission
electron microscopy (TEM), we show the presence of platelet-like nanostructures
in these systems containing Na and/or K. By combining further TEM
and semiclassical theoretical calculations based on a modified Debye
model of the lattice thermal conductivity, we explain the lack of
efficacy of these nanostructures for strong phonon scattering. These
findings are important in the understanding of alkali metals as carriers
in p-type lead chalcogenides. These results also underscore that not
all nanostructures favorably scatter phonons in a matrix; an insight
that may help in further improvements of the power factor and the
overall figure of merit
High Thermoelectric Performance Realized in a BiCuSeO System by Improving Carrier Mobility through 3D Modulation Doping
We
report a greatly enhanced thermoelectric performance in a BiCuSeO
system, realized by improving carrier mobility through modulation
doping. The heterostructures of the modulation doped sample make charge
carriers transport preferentially in the low carrier concentration
area, which increases carrier mobility by a factor of 2 while maintaining
the carrier concentration similar to that in the uniformly doped sample.
The improved electrical conductivity and retained Seebeck coefficient
synergistically lead to a broad, high power factor ranging from 5
to 10 μW cm<sup>–1</sup> K<sup>–2</sup>. Coupling
the extraordinarily high power factor with the extremely low thermal
conductivity of ∼0.25 W m<sup>–1</sup> K<sup>–1</sup> at 923 K, a high <i>ZT</i> ≈ 1.4 is achieved in
a BiCuSeO system
Highly Enhanced Thermoelectric Properties of Bi/Bi<sub>2</sub>S<sub>3</sub> Nanocomposites
Bismuth
sulfide (Bi<sub>2</sub>S<sub>3</sub>) has been of high
interest for thermoelectric applications due to the high abundance
of sulfur on Earth. However, the low electrical conductivity of pristine
Bi<sub>2</sub>S<sub>3</sub> results in a low figure of merit (ZT).
In this work, Bi<sub>2</sub>S<sub>3</sub>@Bi core–shell nanowires
with different Bi shell thicknesses were prepared by a hydrothermal
method. The core–shell nanowires were densified to Bi/Bi<sub>2</sub>S<sub>3</sub> nanocomposite by spark plasma sintering (SPS),
and the structure of the nanowire was maintained as the nanocomposite
due to rapid SPS processing and low sintering temperature. The thermoelectric
properties of bulk samples were investigated. The electrical conductivity
of a bulk sample after sintering at 673 K for 5 min using Bi<sub>2</sub>S<sub>3</sub>@Bi nanowire powders prepared by treating Bi<sub>2</sub>S<sub>3</sub> nanowires in a hydrazine solution for 3 h is 3 orders
of magnitude greater than that of a pristine Bi<sub>2</sub>S<sub>3</sub> sample. The nanocomposite possessed the highest ZT value of 0.36
at 623 K. This represents a new strategy for densifying core–shell
powders to enhance their thermoelectric properties
Energetics of Nanoparticle Exsolution from Perovskite Oxides
The presence of active metal nanoparticles
on the surface significantly
increases the electrochemical performance of ABO<sub>3</sub> perovskite
oxide materials. While conventional deposition methods can improve
the activity, <i>in situ</i> exsolution produces nanoparticles
with far greater stability. The migration of transition metal atoms
toward the surface is expected to affect the exsolution process. To
study the energetics, we use <i>ab initio</i> computations
combined with experiments in a SrTiO<sub>3</sub>-based model system.
Our calculations show that Ni preferentially segregates toward the
(100)-oriented and SrTiO-terminated surfaces, note that this orientation
is identical to one reported by the Irvine and Gorte groups. Vacancies
in the Sr-site and O-site promote the segregation of Ni, while placing
La on the Sr-site has an opposite effect. The corresponding experiments
are in agreement with the computational predictions. Fast nanoparticle
growth and activity enhancement are found in STO system with Sr vacancies
and without La. The approach developed in this Letter could be used
to study the mechanism of exsolution in other material systems, and
possibly lead to the development of new compositions capable of nanoparticle
exsolution with higher activity and stability
Raising the Thermoelectric Performance of p‑Type PbS with Endotaxial Nanostructuring and Valence-Band Offset Engineering Using CdS and ZnS
We have investigated in detail the effect of CdS and
ZnS as second
phases on the thermoelectric properties of p-type PbS. We report a <i>ZT</i> of ∼1.3 at 923 K for 2.5 at.% Na-doped p-type
PbS with endotaxially nanostructured 3.0 at.% CdS. We attribute the
high <i>ZT</i> to the combination of broad-based phonon
scattering on multiple length scales to reduce (lattice) thermal conductivity
and favorable charge transport through coherent interfaces between
the PbS matrix and metal sulfide nanophase precipitates, which maintains
the
requisite high carrier conductivity and the associated power factor.
Similar to large ionically bonded metal sulfides (ZnS, CaS, and SrS),
the covalently bonded CdS can also effectively reduce the lattice
thermal conductivity in p-type PbS. The presence of ubiquitous nanostructuring
was confirmed by transmission electron microscopy. Valence and conduction
band energy levels of the NaCl-type metal sulfides, MS (M = Pb, Cd,
Zn, Ca, and Sr) were calculated from density functional theory to
gain insight into the band alignment between PbS and the second phases
in these materials. The hole transport is controlled by band offset
minimization through the alignment of valence bands between the host
PbS and the embedded second phases, MS (M = Cd, Zn, Ca, and Sr). The
smallest valence band offset of about 0.13 eV at 0 K was found between
PbS and CdS which is diminished further by thermal band broadening
at elevated temperature. This allows carrier transport between the
endotaxially aligned components (i.e., matrix and nanostructure),
thus minimizing significant deterioration of the hole mobility and
power factor. We conclude the thermoelectric performance of the PbS
system and, by extension, other systems can be enhanced by means of
a closely coupled phonon-blocking/electron-transmitting approach through
embedding endotaxially nanostructured second phases
Substrateless Welding of Self-Assembled Silver Nanowires at Air/Water Interface
Integrating
connected silver nanowire networks with flexible polymers has appeared
as a popular way to prepare flexible electronics. To reduce the contact
resistance and enhance the connectivity between silver nanowires,
various welding techniques have been developed. Herein, rather than
welding on solid supporting substrates, which often requires complicated
transferring operations and also may pose damage to heat-sensitive
substrates, we report an alternative approach to prepare easily transferrable
conductive networks through welding of self-assembled silver nanowires
at the air/water interface using plasmonic heating. The intriguing
welding behavior of partially aligned silver nanowires was analyzed
with combined experimental observation and theoretical modeling. The
underlying water not only physically supports the assembled silver
nanowires but also buffers potential overheating during the welding
process, thereby enabling effective welding within a broad range of
illumination power density and illumination duration. The welded networks
could be directly integrated with PDMS substrates to prepare high-performance
stable flexible heaters that are stretchable, bendable, and can be
easily patterned to explore selective heating applications
Thermoelectrics with Earth Abundant Elements: High Performance p-type PbS Nanostructured with SrS and CaS
We report high thermoelectric performance in nanostructured
p-type
PbS, a material consisting of highly earth abundant and inexpensive
elements. The high level of Na doping switched intrinsic n-type PbS
to p-type and substantially raised the power factor maximum for pure
PbS to ∼9.0 μW cm<sup>–1</sup> K<sup>–2</sup> at >723 K using 2.5 at. % Na as the hole dopant. Contrary to
that
of PbTe, no enhancement in the Hall coefficient occurs at high temperature
for heavily doped p-type PbS, indicating a single band model and no
heavy hole band. We also report that the lattice thermal conductivity
of PbS can be greatly reduced by adding SrS or CaS, which form a combination
of a nanostructured/solid solution material as determined by transmission
electron microscopy. We find that both nanoscale precipitates and
point defects play an important role in reducing the lattice thermal
conductivity, but the contribution from nanoscale precipitates of
SrS is greater than that of CaS, whereas the contribution from point
defects in the case of CaS is greater than that of SrS. Theoretical
calculations of the lattice thermal conductivity based on the modified
Callaway model reveal that both nanostructures and point defects (solid
solution) effectively scatter phonons in this system. The lattice
thermal conductivity at 723 K can be reduced by ∼50% by introducing
up to 4.0 at. % of either SrS or CaS. As a consequence, <i>ZT</i> values as high as 1.22 and 1.12 at 923 K can be achieved for nominal
Pb<sub>0.975</sub>Na<sub>0.025</sub>S with 3.0 at. % SrS and CaS,
respectively. No deterioration was observed after a 15 d annealing
treatment of the samples, indicating the excellent thermal stability
for these high performance thermoelectrics. The promising thermoelectric
properties of nanostructured PbS point to a robust low cost alternative
to other high performance thermoelectric materials
Understanding Phonon Scattering by Nanoprecipitates in Potassium-Doped Lead Chalcogenides
We
present a comprehensive experimental and theoretical study of phonon
scattering by nanoprecipitates in potassium-doped PbTe, PbSe, and
PbS. We highlight the role of the precipitate size distribution measured
by microscopy, whose tuning allows for thermal conductivities lower
than the limit achievable with a single size. The correlation between
the size distribution and the contributions to thermal conductivity
from phonons in different frequency ranges provides a physical basis
to the experimentally measured thermal conductivities, and a criterion
to estimate the lowest achievable thermal conductivity. The results
have clear implications for efficiency enhancements in nanostructured
bulk thermoelectrics