2 research outputs found
Role of Point Defects in Spinel Mg Chalcogenide Conductors
Close-packed
chalcogenide spinels, such as MgSc<sub>2</sub>Se<sub>4</sub>, MgIn<sub>2</sub>S<sub>4</sub>, and MgSc<sub>2</sub>S<sub>4</sub>, show potential
as solid electrolytes in Mg batteries, but
are affected by non-negligible electronic conductivity, which contributes
to self-discharge when used in an electrochemical storage device.
Using first-principles calculations, we evaluate the energy of point
defects as a function of synthesis conditions and Fermi level to identify
the origins of the undesired electronic conductivity. Our results
suggest that Mg-vacancies and Mg-metal antisites (where Mg is exchanged
with Sc or In) are the dominant point defects that can occur in the
systems under consideration. While we find anion-excess conditions
and slow cooling to likely create conditions for low electronic conductivity,
the spinels are likely to exhibit significant n-type conductivity
under anion-poor environments, which are often present during high-temperature
synthesis. Finally, we explore extrinsic aliovalent doping to potentially
mitigate the electronic conductivity in these chalcogenide spinels.
The computational strategy is general and can be easily extended to
other solid electrolytes (and electrodes) to aid the optimization
of the electronic properties of the corresponding frameworks
Bistable Amphoteric Native Defect Model of Perovskite Photovoltaics
The past few years
have witnessed unprecedented rapid improvement
of the performance of a new class of photovoltaics based on halide
perovskites. This progress has been achieved even though there is
no generally accepted mechanism of the operation of these solar cells.
Here we present a model based on bistable amphoteric native defects
that accounts for all key characteristics of these photovoltaics and
explains many idiosyncratic properties of halide perovskites. We show
that a transformation between donor-like and acceptor-like configurations
leads to a resonant interaction between amphoteric defects and free
charge carriers. This interaction, combined with the charge transfer
from the perovskite to the electron and hole transporting layers results
in the formation of a dynamic <i>n-i-p</i> junction whose
photovoltaic parameters are determined by the perovskite absorber.
The model provides a unified explanation for the outstanding properties
of the perovskite photovoltaics, including hysteresis of <i>J–V</i> characteristics and ultraviolet light-induced degradation