4 research outputs found
Factors Contributing to Path Hysteresis of Displacement and Conversion Reactions in Li Ion Batteries
We
investigate the thermodynamic and kinetic attributes of electrode
materials that are necessary to suppress path hysteresis during displacement
and conversion reactions in Li ion batteries. We focus on compounds
in the Li–Cu–Sb ternary composition space, as the displacement
reaction between Li<sub>1+ϵ</sub>Cu<sub>1+δ</sub>Sb and
Li<sub>3</sub>Sb can be cycled reversibly. A first-principles analysis
of migration barriers indicates that Cu, while not as mobile as Li
in the discharged phase (Li<sub>3</sub>Sb), nevertheless should exhibit
mobilities similar to that of Li in common intercalation compounds.
A calculation of phase stability in the ternary Li–Cu–Sb
system predicts that the intermediate phases along the reversible
charge/discharge path are stable in a large Cu chemical potential
window. This ensures that intermediate phases are not bypassed upon
Li extraction even when large thermodynamic driving forces are needed
to reinsert Cu into the discharged electrode. Our study suggests that
the suppression of path hysteresis during displacement reactions requires
(i) a high mobility of the displaced metal and (ii) the thermodynamic
stability of intermediate phases along the reversible path in a wide
metal chemical potential window. Even in the absence of path hysteresis,
displacement and conversion reactions suffer from polarization needed
to set up thermodynamic driving forces for metal extrusion and reinsertion.
This polarization can be estimated with a Clausius–Clapeyron
analysis
Accordion Strain Accommodation Mechanism within the Epitaxially Constrained Electrode
The tremendous benefits
of all-solid-state Li-ion batteries will
only be reaped if the cycle-induced strain mismatch across the electrode/electrolyte
interfaces can be managed at the atomic scale to ensure that structural
coherency is maintained over the lifetime of the battery. We have
discovered a unique strain accommodation mechanism within an epitaxially
constrained high-performance bronze TiO<sub>2</sub> (TiO<sub>2</sub>-B) electrode that relieves coherency stresses that arise upon Li
insertion. In situ transmission electron microscopy observation reveals
the formation of anatase shear bands within the TiO<sub>2</sub>-B
crystal that play the same role that interface dislocations do to
relieve growth stresses. While first-principles calculations indicate
that anatase is the favored crystal structure of TiO<sub>2</sub> in
the lithiated state, its continued propagation is suppressed by the
epitaxial constraints of the substrate. This discovery reveals an
accordion-like mechanism relying on an otherwise undesirable structural
transformation that can be exploited to manage the cyclic strain mismatch
across the electrode/electrolyte interfaces that plague all solid-state
batteries
Native Defects in Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> and Their Effect on Lithium Diffusion
Defects
in crystals alter the intrinsic nature of pristine materials
including their electronic/crystalline structure and charge-transport
characteristics. The ionic transport properties of solid-state ionic
conductors, in particular, are profoundly affected by their defect
structure. Nevertheless, a fundamental understanding of the defect
structure of one of the most extensively studied lithium superionic
conductors, Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub>, remains
elusive because of the complexity of the structure; the effects of
defects on lithium diffusion and the potential to control defects
by varying synthetic conditions also remain unknown. Herein, we report,
for the first time, a comprehensive first-principles study on native
defects in Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> and their
effect on lithium diffusion. We provide the complete defect profile
of Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> and identify major
defects that are easily formed regardless of the chemical environment
while the presence of path-blocking defects is sensitively dependent
on the synthetic conditions. Moreover, using <i>ab initio</i> molecular dynamics simulation, it is demonstrated that the major
defects in Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> significantly
alter the diffusion process. The defects generally facilitate lithium
diffusion in Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> by enhancing
the charge carrier concentration and flattening the site energy landscape.
This work delivers a comprehensive picture of the defect chemistry
and structural insights for fast lithium diffusion of Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub>-type conductors
Ionic Conduction in Cubic Na<sub>3</sub>TiP<sub>3</sub>O<sub>9</sub>N, a Secondary Na-Ion Battery Cathode with Extremely Low Volume Change
It is demonstrated that Na ions are
mobile at room temperature
in the nitridophosphate compound Na<sub>3</sub>TiP<sub>3</sub>O<sub>9</sub>N, with a diffusion pathway that is calculated to be fully
three-dimensional and isotropic. When used as a cathode in Na-ion
batteries, Na<sub>3</sub>TiP<sub>3</sub>O<sub>9</sub>N has an average
voltage of 2.7 V vs Na<sup>+</sup>/Na and cycles with good reversibility
through a mechanism that appears to be a single solid solution process
without any intermediate plateaus. X-ray and neutron diffraction studies
as well as first-principles calculations indicate that the volume
change that occurs on Na-ion removal is only about 0.5%, a remarkably
small volume change given the large ionic radius of Na<sup>+</sup>. Rietveld refinements indicate that the Na1 site is selectively
depopulated during sodium removal. Furthermore, the refined displacement
parameters support theoretical predictions that the lowest energy
diffusion pathway incorporates the Na1 and Na3 sites while the Na2
site is relatively inaccessible. The measured room temperature ionic
conductivity of Na<sub>3</sub>TiP<sub>3</sub>O<sub>9</sub>N is substantial
(4 × 10<sup>–7</sup> S/cm), though both the strong temperature
dependence of Na-ion thermal parameters and the observed activation
energy of 0.54 eV suggest that much higher ionic conductivities can
be achieved with minimal heating. Excellent thermal stability is observed
for both pristine Na<sub>3</sub>TiP<sub>3</sub>O<sub>9</sub>N and
desodiated Na<sub>2</sub>TiP<sub>3</sub>O<sub>9</sub>N, suggesting
that this phase can serve as a safe Na-ion battery electrode. Moreover,
it is expected that further optimization of the general cubic framework
of Na<sub>3</sub>TiP<sub>3</sub>O<sub>9</sub>N by chemical substitution
will result in thermostable solid state electrolytes with isotropic
conductivities that can function at temperatures near or just above
room temperature