18 research outputs found
Enhanced Multiple Exciton Dissociation from CdSe Quantum Rods: The Effect of Nanocrystal Shape
A unique ability of semiconductor nanocrystals (NCs)
is the generation
and accommodation of multiple excitons through either optical or electric
current pumping. The development and improvement of NC-based optoelectronic
devices that utilize multiple excitons requires the understanding
of multiple exciton dynamics and their efficient conversion to emitted
photons or external charges prior to excitonâexciton annihilation.
Here, we demonstrate that significantly enhanced multiexciton dissociation
efficiency can be achieved in CdSe quantum rods (QRs) compared to
CdSe quantum dots (QDs). Using transient absorption spectroscopy,
we reveal the formation of bound one-dimensional exciton states in
CdSe QRs and that multiple exciton Auger recombination occurs primarily
via excitonâexciton collision. Furthermore, quantum confinement
in the QR radial direction facilitates ultrafast exciton dissociation
by interfacial electron transfer to adsorbed acceptors. Under high
excitation intensity, more than 21 electrons can be transferred from
one CdSe QR to adsorbed methylviologen molecules, greatly exceeding
the multiexciton dissociation efficiency of CdSe QDs
Charging of Quantum Dots by Sulfide Redox Electrolytes Reduces Electron Injection Efficiency in Quantum Dot Sensitized Solar Cells
In quantum dot (QD) sensitized solar
cells (QDSSCs), redox electrolytes
act as hole scavengers to regenerate the QD ground state from its
oxidized form, thus enabling a continuous device operation. However,
unlike molecular sensitizers, QDs also have redox-active trap states
within the band gap, which can be charged in the presence of redox
electrolyte. The effects of electrolyte induced charging of QDs on
the performance of QDSSCs have not been reported. Here, using steady-state
and time-resolved absorption and emission spectroscopy, we show that
CdSe/CdS<sub>3ML</sub>ZnÂCdS<sub>2ML</sub>ZnÂS<sub>2ML</sub> core/multishell QDs are charged in the presence of sulfide electrolytes
due to the reduction of surface states. As a result, exciton lifetimes
in these QDs are shortened due to an Auger recombination process.
Such charging induced fast Auger recombination can compete effectively
with electron transfer from QDs to TiO<sub>2</sub> and reduce the
electron injection efficiency in QDSSCs. We believe that the reported
charging effects are present for most colloidal nanocrystals in the
presence of redox media and have important implications for designing
QD-based photovoltaic and photocatalytic devices
Probing Spatially Dependent Photoinduced Charge Transfer Dynamics to TiO<sub>2</sub> Nanoparticles Using Single Quantum Dot Modified Atomic Force Microscopy Tips
Using
single CdSe/CdS quantum dot (QD) functionalized atomic force
microscopy (AFM) tips, we demonstrate that the spatial dependence
of photoinduced electron transfer dynamics from the single QD to TiO<sub>2</sub> nanoparticles can be controlled and probed with high spatial
(subdiffraction-limited) and temporal (limited by fluorescence microscopy)
resolutions. This finding suggests the feasibility of using electron
donor or acceptor modified AFM tips for simultaneous high resolution
imaging of morphology and photoinduced charge transfer dynamics in
nanomaterials
Beyond Band Alignment: Hole Localization Driven Formation of Three Spatially Separated Long-Lived Exciton States in CdSe/CdS Nanorods
Colloidal one-dimensional semiconductor nanoheterostructures have emerged as an important family of functional materials for solar energy conversion, although the nature of the long-lived exciton state and their formation and dissociation dynamics remain poorly understood. In this paper we study these dynamics in CdSe/CdS dot-in-rod (DIR) NRs, a representative of 1D heterostructures, and DIR-electron-acceptor complexes by transient absorption spectroscopy. Because of a quasi-type II band alignment of CdSe and CdS, it is often assumed that there exists one long-lived exciton state with holes localized in the CdSe seed and electrons delocalized among CdSe and CdS. We show that excitation into the CdS rod forms three distinct types of long-lived excitons that are spatially localized in the CdS rod, in and near the CdSe seed and in the CdS shell surrounding the seed. The branching ratio of forming these exciton states is controlled by the competition between the band offset driven hole localization to the CdSe seed and hole trapping to the CdS surface. Because of dielectric contrast induced strong electronâhole interaction in 1D materials, the competing hole localization pathways lead to spatially separated long-lived excitons. Their distinct spatial locations affect their dissociation rates in the presence of electron acceptors, which has important implications for the application of 1D heterostructures as light-harvesting materials
Ultrafast Charge Separation and Long-Lived Charge Separated State in Photocatalytic CdSâPt Nanorod Heterostructures
Colloidal semiconductorâmetal nanoheterostructures
that
combine the light-harvesting ability of semiconductor nanocrystals
with the catalytic activity of small metal nanoparticles show promising
applications for photocatalysis, including light-driven H<sub>2</sub> production. The exciton in the semiconductor domain can be quenched
by electron-, hole-, and energy transfer to the metal particle, and
the competition between these processes determines the photocatalytic
efficiency of these materials. Using ultrafast transient absorption
spectroscopy, we show that, in CdSâPt heterostructures consisting
of a CdS nanorod with a Pt nanoparticle at one end, the excitons in
the CdS domain dissociate by ultrafast electron transfer (with a half-life
of âŒ3.4 ps) to the Pt. The charge separated state is surprisingly
long-lived (with a half-life of âŒ1.2 ± 0.6 ÎŒs) due
to the trapping of holes in CdS. The asymmetry in the charge separation
and recombination times is believed to be the key feature that enables
the accumulation of the transferred electrons in the Pt tip and photocatalysis
in the presence of sacrificial hole acceptors
Near Unity Quantum Yield of Light-Driven Redox Mediator Reduction and Efficient H<sub>2</sub> Generation Using Colloidal Nanorod Heterostructures
The advancement of direct solar-to-fuel conversion technologies
requires the development of efficient catalysts as well as efficient
materials and novel approaches for light harvesting and charge separation.
We report a novel system for unprecedentedly efficient (with near-unity
quantum yield) light-driven reduction of methylviologen (MV<sup>2+</sup>), a common redox mediator, using colloidal quasi-type II CdSe/CdS
dot-in-rod nanorods as a light absorber and charge separator and mercaptopropionic
acid as a sacrificial electron donor. In the presence of Pt nanoparticles,
this system can efficiently convert sunlight into H<sub>2</sub>, providing
a versatile redox mediator-based approach for solar-to-fuel conversion.
Compared to related CdSe seed and CdSe/CdS core/shell quantum dots
and CdS nanorods, the quantum yields are significantly higher in the
CdSe/CdS dot-in-rod structures. Comparison of charge separation, recombination
and hole filling rates in these complexes showed that the dot-in-rod
structure enables ultrafast electron transfer to methylviologen, fast
hole removal by sacrificial electron donor and slow charge recombination,
leading to the high quantum yield for MV<sup>2+</sup> photoreduction.
Our finding demonstrates that by controlling the composition, size
and shape of quantum-confined nanoheterostructures, the electron and
hole wave functions can be tailored to produce efficient light harvesting
and charge separation materials
Light-Driven, Quantum Dot-Mediated Regeneration of FMN To Drive Reduction of Ketoisophorone by Old Yellow Enzyme
We report the full reduction of the biological cofactor
FMN with
visible light using CdSe quantum dots and methylviologen as an electron
relay. In turn, these reducing equivalents can drive the stereospecific
reduction of ketoisophorone by an old yellow enzyme homologue from Bacillus subtilis (YqjM). The experiments demonstrate
the current capabilities and limitations of quantum dots as part of
a cofactor regeneration system and pave the road for future studies
aimed at new and improved in situ light-driven cofactor regeneration
strategies
Unraveling the Exciton Quenching Mechanism of Quantum Dots on Antimony-Doped SnO<sub>2</sub> Films by Transient Absorption and Single Dot Fluorescence Spectroscopy
Integrating quantum dots (QDs) into modern optoelectronic devices requires an understanding of how a transparent conducting substrate affects the properties of QDs, especially their excited-state dynamics. Here, the exciton quenching dynamics of core/multishell (CdSe/CdS<sub>3ML</sub>ZnCdS<sub>2ML</sub>ZnS<sub>2ML</sub>) quantum dots deposited on glass, tin oxide (SnO<sub>2</sub>), and antimony (Sb)-doped tin oxide (ATO) films are studied by transient absorption and single QD fluorescence spectroscopic methods. By comparing ensemble-averaged fluorescence decay and transient absorption kinetics, we show that, for QDs on SnO<sub>2</sub>, the exciton is quenched by electron transfer from the QD to SnO<sub>2</sub>. At the QDâATO interface, much faster exciton quenching rates are observed and attributed to fast Auger recombination in charged QDs formed by Fermi level equilibration between the QD and n-doped ATO. Single QDs on SnO<sub>2</sub> and ATO show similar blinking dynamics with correlated fluctuations of emission intensities and lifetimes. Compared to QDs on SnO<sub>2</sub>, QDs on ATO films show larger variation of average exciton quenching rates, which is attributed to a broad distribution of the number of charges and nature of charging sites on the QD surface
Interfacial Charge Transfer Circumventing Momentum Mismatch at Two-Dimensional van der Waals Heterojunctions
Interfacial
charge separation and recombination at heterojunctions of monolayer
transition metal dichalcogenides (TMDCs) are of interest to two-dimensional
optoelectronic technologies. These processes can involve large changes
in parallel momentum vector due to the confinement of electrons and
holes to the K valleys in each layer. Because these high-momentum
valleys are usually not aligned across the interface of two TMDC monolayers,
how parallel momentum is conserved in the charge separation or recombination
process becomes a key question. Here we probe this question using
the model system of a type-II heterojunction formed by MoS<sub>2</sub> and WSe<sub>2</sub> monolayers and the experimental technique of
femtosecond pumpâprobe spectroscopy. Upon photoexcitation specifically
of WSe<sub>2</sub> at the heterojunction, we observe ultrafast (<40
fs) electron transfer from WSe<sub>2</sub> to MoS<sub>2</sub>, independent
of the angular alignment and thus momentum mismatch between the two
TMDCs. The resulting interlayer charge transfer exciton decays via
nonradiative recombination with rates varying by up to three-orders
of magnitude from sample to sample but with no correlation with interlayer
angular alignment. We suggest that the initial interfacial charge
separation and the subsequent interfacial charge recombination processes
circumvent momentum mismatch via excess electronic energy and via
defect-mediated recombination, respectively
Hole Removal Rate Limits Photodriven H<sub>2</sub> Generation Efficiency in CdS-Pt and CdSe/CdS-Pt Semiconductor NanorodâMetal Tip Heterostructures
Semiconductorâmetal
nanoheterostructures, such as CdSe/CdS
dot-in-rod nanorods with a Pt tip at one end (or CdSe/CdS-Pt), are
promising materials for solar-to-fuel conversion because they allow
rational integration of a light absorber, hole acceptor, and electron
acceptor or catalyst in an all-inorganic triadic heterostructure as
well as systematic control of relative energetics and spatial arrangement
of the functional components. To provide design principles of such
triadic nanorods, we examined the photocatalytic H<sub>2</sub> generation
quantum efficiency and the rates of elementary charge separation and
recombination steps of CdSe/CdS-Pt and CdS-Pt nanorods. We showed
that the steady-state H<sub>2</sub> generation quantum efficiencies
(QEs) depended sensitively on the electron donors and the nanorods.
Using ultrafast transient absorption spectroscopy, we determined that
the electron transfer efficiencies to the Pt tip were near unity for
both CdS and CdSe/CdS nanorods. Hole transfer rates to the electron
donor, measured by time-resolved fluorescence decay, were positively
correlated with the steady-state H<sub>2</sub> generation QEs. These
results suggest that hole transfer is a key efficiency-limiting step.
These insights provide possible ways for optimizing the hole transfer
step to achieve efficient solar-to-fuel conversion in semiconductorâmetal
nanostructures