8 research outputs found
Reaction Heterogeneity in LiNi<sub>0.8</sub>Co<sub>0.15</sub>Al<sub>0.05</sub>O<sub>2</sub> Induced by Surface Layer
Through operando
synchrotron powder X-ray diffraction (XRD) analysis
of layered transition metal oxide electrodes of composition LiNi<sub>0.8</sub>Co<sub>0.15</sub>Al<sub>0.05</sub>O<sub>2</sub> (NCA), we
decouple the intrinsic bulk reaction mechanism from surface-induced
effects. For identically prepared and cycled electrodes stored in
different environments, we demonstrate that the intrinsic bulk reaction
for pristine NCA follows solid-solution mechanism, not a two-phase
as suggested previously. By combining high resolution powder X-ray
diffraction, diffuse reflectance infrared Fourier transform spectroscopy
(DRIFTS), and surface sensitive X-ray photoelectron spectroscopy (XPS),
we demonstrate that adventitious Li<sub>2</sub>CO<sub>3</sub> forms
on the electrode particle surface during exposure to air through reaction
with atmospheric CO<sub>2</sub>. This surface impedes ionic and electronic
transport to the underlying electrode, with progressive erosion of
this layer during cycling giving rise to different reaction states
in particles with an intact versus an eroded Li<sub>2</sub>CO<sub>3</sub> surface-coating. This reaction heterogeneity, with a bimodal
distribution of reaction states, has previously been interpreted as
a “two-phase” reaction mechanism for NCA, as an activation
step that only occurs during the first cycle. Similar surface layers
may impact the reaction mechanism observed in other electrode materials
using bulk probes such as operando powder XRD
Programming Interfacial Energetic Offsets and Charge Transfer in β‑Pb<sub>0.33</sub>V<sub>2</sub>O<sub>5</sub>/Quantum-Dot Heterostructures: Tuning Valence-Band Edges to Overlap with Midgap States
Semiconductor
heterostructures for solar energy conversion interface
light-harvesting semiconductor nanoparticles with wide-band-gap semiconductors
that serve as charge acceptors. In such heterostructures, the kinetics
of charge separation depend on the thermodynamic driving force, which
is dictated by energetic offsets across the interface. A recently
developed promising platform interfaces semiconductor quantum dots
(QDs) with ternary vanadium oxides that have characteristic midgap
states situated between the valence and conduction bands. In this
work, we have prepared CdS/β-Pb<sub>0.33</sub>V<sub>2</sub>O<sub>5</sub> heterostructures by both linker-assisted assembly and surface
precipitation and contrasted these materials with CdSe/β-Pb<sub>0.33</sub>V<sub>2</sub>O<sub>5</sub> heterostructures prepared by
the same methods. Increased valence-band (VB) edge onsets in X-ray
photoelectron spectra for CdS/β-Pb<sub>0.33</sub>V<sub>2</sub>O<sub>5</sub> heterostructures relative to CdSe/β-Pb<sub>0.33</sub>V<sub>2</sub>O<sub>5</sub> heterostructures suggest a positive shift
in the VB edge potential and, therefore, an increased driving force
for the photoinduced transfer of holes to the midgap state of β-Pb<sub>0.33</sub>V<sub>2</sub>O<sub>5</sub>. This approach facilitates a
ca. 0.40 eV decrease in the thermodynamic barrier for hole injection
from the VB edge of QDs suggesting an important design parameter.
Transient absorption spectroscopy experiments provide direct evidence
of hole transfer from photoexcited CdS QDs to the midgap states of
β-Pb<sub>0.33</sub>V<sub>2</sub>O<sub>5</sub> NWs, along with
electron transfer into the conduction band of the β-Pb<sub>0.33</sub>V<sub>2</sub>O<sub>5</sub> NWs. Hole transfer is substantially faster
and occurs at <1-ps time scales, whereas completion of electron
transfer requires 530 ps depending on the nature of the interface.
The differentiated time scales of electron and hole transfer, which
are furthermore tunable as a function of the mode of attachment of
QDs to NWs, provide a vital design tool for designing architectures
for solar energy conversion. More generally, the approach developed
here suggests that interfacing semiconductor QDs with transition-metal
oxide NWs exhibiting intercalative midgap states yields a versatile
platform wherein the thermodynamics and kinetics of charge transfer
can be systematically modulated to improve the efficiency of charge
separation across interfaces
What Happens to LiMnPO<sub>4</sub> upon Chemical Delithiation?
Olivine MnPO<sub>4</sub> is the delithiated
phase of the lithium-ion-battery cathode (positive electrode) material
LiMnPO<sub>4</sub>, which is formed at the end of charge. This phase
is metastable under ambient conditions and can only be produced by
delithiation of LiMnPO<sub>4</sub>. We have revealed the manganese
dissolution phenomenon during chemical delithiation of LiMnPO<sub>4</sub>, which causes amorphization of olivine MnPO<sub>4</sub>.
The properties of crystalline MnPO<sub>4</sub> obtained from carbon-coated
LiMnPO<sub>4</sub> and of the amorphous product resulting from delithiation
of pure LiMnPO<sub>4</sub> were studied and compared. The phosphorus-rich
amorphous phases in the latter are considered to be MnHP<sub>2</sub>O<sub>7</sub> and MnH<sub>2</sub>P<sub>2</sub>O<sub>7</sub> from
NMR, X-ray absorption spectroscopy, and X-ray photoelectron spectroscopy
analysis. The thermal stability of MnPO<sub>4</sub> is significantly
higher under high vacuum than at ambient condition, which is shown
to be related to surface water removal
Mitigating Cation Diffusion Limitations and Intercalation-Induced Framework Transitions in a 1D Tunnel-Structured Polymorph of V<sub>2</sub>O<sub>5</sub>
The
design of cathodes for intercalation batteries requires consideration
of both atomistic and electronic structure to facilitate redox at
specific transition metal sites along with the concomitant diffusion
of cations and electrons. Cation intercalation often brings about
energy dissipative phase transformations that give rise to substantial
intercalation gradients as well as multiscale phase and strain inhomogeneities.
The layered α-V<sub>2</sub>O<sub>5</sub> phase is considered
to be a classical intercalation host but is plagued by sluggish diffusion
kinetics and a series of intercalation-induced phase transitions that
require considerable lattice distortion. Here, we demonstrate that
a 1D tunnel-structured ζ-phase polymorph of V<sub>2</sub>O<sub>5</sub> provides a stark study in contrast and can reversibly accommodate
Li-ions without a large distortion of the structural framework and
with substantial mitigation of polaronic confinement. Entirely homogeneous
lithiation is evidenced across multiple cathode particles (in contrast
to α-V<sub>2</sub>O<sub>5</sub> particles wherein lithiation-induced
phase transformations induce phase segregation). Barriers to Li-ion
as well as polaron diffusion are substantially diminished for metastable
ζ-V<sub>2</sub>O<sub>5</sub> in comparison to the thermodynamically
stable α-V<sub>2</sub>O<sub>5</sub> phase. The rigid tunnel
framework, relatively small changes in coordination environment of
intercalated Li-ions across the diffusion pathways defined by the
1D tunnels, and degeneracy of V 3d states at the bottom of the conduction
band reduce electron localization that is a major impediment to charge
transport in α-V<sub>2</sub>O<sub>5</sub>. The 1D ζ-phase
thus facilitates a continuous lithiation pathway that is markedly
different from the successive intercalation-induced phase transitions
observed in α-V<sub>2</sub>O<sub>5</sub>. The results here illustrate
the importance of electronic structure in mediating charge transport
in oxide cathode materials and demonstrates that a metastable polymorph
with higher energy bonding motifs that define frustrated coordination
environments can serve as an attractive intercalation host
Mitigating Cation Diffusion Limitations and Intercalation-Induced Framework Transitions in a 1D Tunnel-Structured Polymorph of V<sub>2</sub>O<sub>5</sub>
The
design of cathodes for intercalation batteries requires consideration
of both atomistic and electronic structure to facilitate redox at
specific transition metal sites along with the concomitant diffusion
of cations and electrons. Cation intercalation often brings about
energy dissipative phase transformations that give rise to substantial
intercalation gradients as well as multiscale phase and strain inhomogeneities.
The layered α-V<sub>2</sub>O<sub>5</sub> phase is considered
to be a classical intercalation host but is plagued by sluggish diffusion
kinetics and a series of intercalation-induced phase transitions that
require considerable lattice distortion. Here, we demonstrate that
a 1D tunnel-structured ζ-phase polymorph of V<sub>2</sub>O<sub>5</sub> provides a stark study in contrast and can reversibly accommodate
Li-ions without a large distortion of the structural framework and
with substantial mitigation of polaronic confinement. Entirely homogeneous
lithiation is evidenced across multiple cathode particles (in contrast
to α-V<sub>2</sub>O<sub>5</sub> particles wherein lithiation-induced
phase transformations induce phase segregation). Barriers to Li-ion
as well as polaron diffusion are substantially diminished for metastable
ζ-V<sub>2</sub>O<sub>5</sub> in comparison to the thermodynamically
stable α-V<sub>2</sub>O<sub>5</sub> phase. The rigid tunnel
framework, relatively small changes in coordination environment of
intercalated Li-ions across the diffusion pathways defined by the
1D tunnels, and degeneracy of V 3d states at the bottom of the conduction
band reduce electron localization that is a major impediment to charge
transport in α-V<sub>2</sub>O<sub>5</sub>. The 1D ζ-phase
thus facilitates a continuous lithiation pathway that is markedly
different from the successive intercalation-induced phase transitions
observed in α-V<sub>2</sub>O<sub>5</sub>. The results here illustrate
the importance of electronic structure in mediating charge transport
in oxide cathode materials and demonstrates that a metastable polymorph
with higher energy bonding motifs that define frustrated coordination
environments can serve as an attractive intercalation host
Visible Light-Driven H<sub>2</sub> Production over Highly Dispersed Ruthenia on Rutile TiO<sub>2</sub> Nanorods
The immobilization of miniscule quantities
of RuO<sub>2</sub> (∼0.1%)
onto one-dimensional (1D) TiO<sub>2</sub> nanorods (NRs) allows H<sub>2</sub> evolution from water under visible light irradiation. Rod-like
rutile TiO<sub>2</sub> structures, exposing preferentially (110) surfaces,
are shown to be critical for the deposition of RuO<sub>2</sub> to
enable photocatalytic activity in the visible region. The superior
performance is rationalized on the basis of fundamental experimental
studies and theoretical calculations, demonstrating that RuO<sub>2</sub>(110) grown as 1D nanowires on rutile TiO<sub>2</sub>(110), which
occurs only at extremely low loads of RuO<sub>2</sub>, leads to the
formation of a heterointerface that efficiently adsorbs visible light.
The surface defects, band gap narrowing, visible photoresponse, and
favorable upward band bending at the heterointerface drastically facilitate
the transfer and separation of photogenerated charge carriers
Electrochemical Performance of Nanosized Disordered LiVOPO<sub>4</sub>
ε-LiVOPO<sub>4</sub> is a promising multielectron cathode
material for Li-ion batteries that can accommodate two electrons per
vanadium, leading to higher energy densities. However, poor electronic
conductivity and low lithium ion diffusivity currently result in low
rate capability and poor cycle life. To enhance the electrochemical
performance of ε-LiVOPO<sub>4</sub>, in this work, we optimized
its solid-state synthesis route using in situ synchrotron X-ray diffraction
and applied a combination of high-energy ball-milling with electronically
and ionically conductive coatings aiming to improve bulk and surface
Li diffusion. We show that high-energy ball-milling, while reducing
the particle size also introduces structural disorder, as evidenced
by <sup>7</sup>Li and <sup>31</sup>P NMR and X-ray absorption spectroscopy.
We also show that a combination of electronically and ionically conductive
coatings helps to utilize close to theoretical capacity for ε-LiVOPO<sub>4</sub> at C/50 (1 C = 153 mA h g<sup>–1</sup>) and to enhance
rate performance and capacity retention. The optimized ε-LiVOPO<sub>4</sub>/Li<sub>3</sub>VO<sub>4</sub>/acetylene black composite yields
the high cycling capacity of 250 mA h g<sup>–1</sup> at C/5
for over 70 cycles