4 research outputs found
Grain Boundaries Are Benign and Suppress Nonradiative Electron–Hole Recombination in Monolayer Black Phosphorus: A Time-Domain Ab Initio Study
Using
time-domain density functional theory combined with nonadiabatic
molecular dynamics, we demonstrate that both symmetrical (GB_s) and
asymmetrical grain boundaries (GB_a) significantly extend charge-carrier
lifetime compared with monolayer black phosphorus. Boundaries create
no deep trap states, which decrease electron–phonon coupling.
As a result, GB_s increases carrier lifetime by a factor of 22, whereas
GB_a extends the lifetime by a factor of 4. More importantly, the
interplay between the immobile electron localized at the boundaries
in the GB_s and extended excited-state lifetime facilitates a chemical
reaction, which is beneficial for photocatalysts. In contrast, GB_a
separates electron and hole spatially in different locations, which
forms a long-lived charge-separated state and is favorable for photovoltaics.
Our simulations demonstrate that grain boundaries are benign and retard
nonradiative electron–hole recombination in monolayer black
phosphorus, suggesting a route to reduce energy losses via rational
choice of defect to realize high-performance photovoltaic and photocatalytic
devices
Defects Slow Down Nonradiative Electron–Hole Recombination in TiS<sub>3</sub> Nanoribbons: A Time-Domain Ab Initio Study
Layered TiS<sub>3</sub> materials hold appealing potential in photovoltaics
and optoelectronics due to their excellent electronic and optical
properties. Using time domain density functional theory combined with
nonadiabatic (NA) molecular dynamics, we show that the electron–hole
recombination in pristine TiS<sub>3</sub> nanoribbons (NRs) occurs
in tens of picoseconds and is over 10-fold faster than the experimental
value. By performing an atomistic ab initio simulation with a sulfur
vacancy, we demonstrate that a sulfur vacancy greatly reduces electron–hole
recombination, achieving good agreement with experiment. Introduction
of a sulfur vacancy increases the band gap slightly because the NR’s
highest occupied molecular orbital is lowered in energy. More importantly,
the sulfur vacancy partially diminishes the electron and hole wave
functions’ overlap and reduces NA electron–phonon coupling,
which competes successfully with the longer decoherence time, slowing
down recombination. Our study suggests that a rational choice of defects
can control nonradiative electron–hole recombination in TiS<sub>3</sub> NRs and provides mechanistic principles for photovoltaic
and optoelectronic device design
Nonadiabatic Molecular Dynamics Simulation of Charge Separation and Recombination at a WS<sub>2</sub>/QD Heterojunction
Two-dimensional transition
metal dichalcogenides (TMDs), such as
WS<sub>2</sub>, are appealing candidates for optoelectronics and photovoltaics.
The strong Coulomb interaction in TMDs is however known to prevent
electron–hole pairs from dissociating into free electron and
hole. The experiment demonstrates that combination of WS<sub>2</sub> and quantum dots (QDs) can achieve efficient charge separation and
enhance photon-to-electron conversion efficiency. Using real-time
time-dependent density functional theory combined with nonadiabatic
molecular dynamics, we model electron and hole transfer dynamics at
a WS<sub>2</sub>/QD heterojunction. We demonstrate that both electron
and hole transfer are ultrafast due to strong donor–acceptor
coupling. The photoexcitation of the WS<sub>2</sub> leads to a 75
fs electron transfer, followed by a 0.45 eV loss within 90 fs. The
photoexcitation of QD results in 240 fs hole transfer, but loses only
0.15 eV of energy within 1 ps. The strong charge–phonon coupling
and a broad range of phonon modes involved in electron dynamics are
responsible for the faster electron transfer than the hole transfer.
The electron–hole recombination across the WS<sub>2</sub>/QD
interface occurs in several 100 ps, ensuing a long-lived charge-separated
state. Particularly, the hole transfer is threefold magnitude faster
than the electron–hole recombination inside QD, ensuing that
QD can be an excellent light-harvester. The detailed atomistic insights
into the photoinduced charge and energy dynamics at the WS<sub>2</sub>/QD interface provide valuable guidelines for the optimization of
solar light-harvesting and photovoltaic efficiency in modern nanoscale
materials
Tunnel-Structured K<sub><i>x</i></sub>TiO<sub>2</sub> Nanorods by in Situ Carbothermal Reduction as a Long Cycle and High Rate Anode for Sodium-Ion Batteries
The
low electronic conductivity and the sluggish sodium-ion diffusion
in the compact crystal structure of Ti-based anodes seriously restrict
their development in sodium-ion batteries. In this study, a new hollandite
K<sub><i>x</i></sub>TiO<sub>2</sub> with large (2 Ă—
2) tunnels is synthesized by a facile carbothermal reduction method,
and its sodium storage performance is investigated. X-ray diffraction
(XRD) and transmission electron microscopy (TEM) analyses illustrate
the formation mechanism of the hollandite K<sub><i>x</i></sub>TiO<sub>2</sub> upon the carbothermal reduction process. Compared
to the traditional layered or small (1 Ă— 1) tunnel-type Ti-based
materials, the hollandite K<sub><i>x</i></sub>TiO<sub>2</sub> with large (2 Ă— 2) tunnels may accommodate more sodium ions
and facilitate the Na<sup>+</sup> diffusion in the structure; thus,
it is expected to get a large capacity and realize high rate capability.
The synthesized K<sub><i>x</i></sub>TiO<sub>2</sub> with
large (2 Ă— 2) tunnels shows a stable reversible capacity of 131
mAh g<sup>–1</sup> (nearly 3 times of (1 × 1) tunnel-structured
Na<sub>2</sub>Ti<sub>6</sub>O<sub>13</sub>) and superior cycling stability
with no obvious capacity decay even after 1000 cycles, which is significantly
better than the traditional layered Na<sub>2</sub>Ti<sub>3</sub>O<sub>7</sub> (only 40% of capacity retention in 20 cycles). Moreover,
the carbothermal process can naturally introduce oxygen vacancy and
low-valent titanium as well as the surface carbon coating layer to
the structure, which would greatly enhance the electronic conductivity
of K<sub><i>x</i></sub>TiO<sub>2</sub> and thus endow this
material high rate capability. With a good rate capability and long
cyclability, this hollandite K<sub><i>x</i></sub>TiO<sub>2</sub> can serve as a new promising anode material for room-temperature
long-life sodium-ion batteries for large-scale energy storage systems,
and the carbothermal reduction method is believed to be an effective
and facile way to develop novel Ti-based anodes with simultaneous
carbon coating and TiÂ(III) self-doping