8 research outputs found
Layer-by-Layer Self-Assembly of CdS Quantum Dots/Graphene Nanosheets Hybrid Films for Photoelectrochemical and Photocatalytic Applications
In
recent years, increasing interest has been devoted to synthesizing
graphene–semiconductor nanocomposites as efficient photocatalysts
for extensive applications. Unfortunately, it is still challenging
to make uniform graphene–semiconductor composite films with
controllable film thickness and architecture, which are of paramount
importance to meet the application requirements. In this work, stable
aqueous dispersion of polymer-modified graphene nanosheets (GNs) was
prepared via in situ reduction of exfoliated graphite oxide in the
presence of cationic polyÂ(allylamine hydrochloride) (PAH). The resultant
water-soluble PAH-modified GNs (GNs-PAH) in conjunction with tailor-made
negatively charged CdS quantum dots (QDs) were utilized as nanobuilding
blocks for sequential layer-by-layer (LbL) self-assembly of well-defined
GNs–CdS QDs hybrid films, in which CdS QDs overspread evenly
on the two-dimensional (2D) GNs. It was found that the alternating
GNs–CdS QDs multilayered films showed significantly enhanced
photoelectrochemical and photocatalytic activities under visible light
irradiation as compared to pure CdS QDs and GNs films. The enhancement
was attributed to the judicious integration of CdS QDs with GNs in
an alternating manner, which maximizes the 2D structural advantage
of GNs in GNs–CdS QDs composite films. In addition, photocatalytic
and photoelectrochemical mechanisms of the GNs–CdS QDs multilayered
films were also discussed. It is anticipated that our work may open
new directions for the fabrication of uniform semiconductor/GNs hybrid
films for a wide range of applications
Thermodynamically Driven One-Dimensional Evolution of Anatase TiO<sub>2</sub> Nanorods: One-Step Hydrothermal Synthesis for Emerging Intrinsic Superiority of Dimensionality
In
photoelectrochemical cells, there exists a competition between
transport of electrons through the porous semiconductor electrode
toward the conducting substrate and back-reaction of electrons to
recombine with oxidized species on the semiconductor–electrolyte
interface, which determines the charge collection efficiency and is
strongly influenced by the density and distribution of electronic
states in band gap and architectures of the semiconductor electrodes.
One-dimensional (1D) anatase TiO<sub>2</sub> nanostructures are promising
to improve charge transport in photoelectrochemical devices. However,
the conventional preparation of 1D anatase nanostructures usually
steps via a titanic acid intermediate (e.g., H<sub>2</sub>Ti<sub>3</sub>O<sub>7</sub>), which unavoidably introduces electronic defects into
the host lattice, resulting in undesired shielding of the intrinsic
role of dimensionality. Here, we manage to promote the 1D growth of
anatase TiO<sub>2</sub> nanostructures by adjusting the growth kinetics,
which allows us to grow single-crystalline anatase TiO<sub>2</sub> nanorods through a one-step hydrothermal reaction. The synthesized
anatase nanorods possess a lower density of trap states and thus can
simultaneously facilitate the diffusion-driven charge transport and
suppress the electron recombination. Moreover, the electronically
boundary free nanostructures significantly enhance the trap-free charge
diffusion coefficient of the anatase nanorods, which enables the emergence
of the intrinsic superiority of dimensionality. By virtue of these
merits, the anatase nanorods synthesized in this work take obvious
advantages over the conventional anatase counterparts in photoelectrochemical
systems (e.g., dye-sensitized solar cells) by showing more efficient
charge transport and collection and higher energy conversion efficiency
Understanding Chemical Bonding in Alloys and the Representation in Atomistic Simulations
Alloys
are widely used in catalysts and structural materials. The
nature of chemical bonding and the origin of alloy formation energies,
defect energies, and interfacial properties have not been well understood
to date but are critical to material performance. In this contribution,
we explain the polar nature of chemical bonding and an implementation
in classical and reactive atomistic simulations to understand such
properties more quantitatively. Electronegativity differences between
metal atoms lead to polar bonding, and exothermic alloy formation
energies are related to charge transfer between the different elements.
These differences can be quantified by atomic charges using pairwise
charge increments, determined by matching the computed alloy
formation energy to experimentally measured alloy formation energies
using pair potentials for the pure metals. The polar character of
alloys is comparable to organic molecules and partially ionic minerals,
for example, AlNi and AlNi<sub>3</sub> alloys assume significant atomic
charges of ±0.40<i>e</i> and +0.60<i>e</i>/–0.20<i>e</i>, respectively. The subsequent analysis
of defect sites and defect energies using force-field-based calculations
shows excellent agreement with calculations using density functional
theory and embedded atom models (EAM). The formation of vacancy and
antisite defects is characterized by a redistribution of charge in
the first shell of neighbor atoms in the classical models whereby
electroneutrality is maintained and charge increments correlate with
differences in electronegativity. The proposed atomic charges represent
internal dipole and multipole moments, consistent with existing definitions
for organic and inorganic compounds and with the extended Born model
(Heinz, H.; Suter, U. W. <i>J. Phys. Chem. B</i> <b>2004,</b> <i>108</i> (47), 18341–18352). The method can be
applied to any alloy and has a reproducibility of ±10%. In contrast,
quantum mechanical charge schemes remain associated with deviations
exceeding ±100%. The atomic charges for alloys provide a simple
initial measure for the internal electronic structure, surface adsorption
of molecules, and reactivity in catalysis and corrosion. The models
are compatible with the Interface force field (IFF), CHARMM, AMBER,
OPLS-AA, PCFF, CVFF, and GROMOS for reliable atomistic simulations
of alloys and their interfaces with minerals and electrolytes from
the nanometer scale to the micrometer scale
Stable Quantum Dot Photoelectrolysis Cell for Unassisted Visible Light Solar Water Splitting
Sunlight is an ideal source of energy, and converting sunlight into chemical fuels, mimicking what nature does, has attracted significant attention in the past decade. In terms of solar energy conversion into chemical fuels, solar water splitting for hydrogen production is one of the most attractive renewable energy technologies, and this achievement would satisfy our increasing demand for carbon-neutral sustainable energy. Here, we report corrosion-resistant, nanocomposite photoelectrodes for spontaneous overall solar water splitting, consisting of a CdS quantum dot (QD) modified TiO<sub>2</sub> photoanode and a CdSe QD modified NiO photocathode, where cadmium chalcogenide QDs are protected by a ZnS passivation layer and gas evolution cocatalysts. The optimized device exhibited a maximum efficiency of 0.17%, comparable to that of natural photosynthesis with excellent photostability under visible light illumination. Our device shows spontaneous overall water splitting in a nonsacrificial environment under visible light illumination (λ > 400 nm) through mimicking nature’s “Z-scheme” process. The results here also provide a conceptual layout to improve the efficiency of solar-to-fuel conversion, which is solely based on facile, scalable solution-phase techniques
Identification of Surface Reactivity Descriptor for Transition Metal Oxides in Oxygen Evolution Reaction
A number of important
reactions such as the oxygen evolution reaction
(OER) are catalyzed by transition metal oxides (TMOs), the surface
reactivity of which is rather elusive. Therefore, rationally tailoring
adsorption energy of intermediates on TMOs to achieve desirable catalytic
performance still remains a great challenge. Here we show the identification
of a general and tunable surface structure, coordinatively unsaturated
metal cation (M<sub>CUS</sub>), as a good surface reactivity descriptor
for TMOs in OER. Surface reactivity of a given TMO increases monotonically
with the density of M<sub>CUS</sub>, and thus the increase in M<sub>CUS</sub> improves the catalytic activity for weak-binding TMOs but
impairs that for strong-binding ones. The electronic origin of the
surface reactivity can be well explained by a new model proposed in
this work, wherein the energy of the highest-occupied d-states relative
to the Fermi level determines the intermediates’ bonding strength
by affecting the filling of the antibonding states. Our model for
the first time well describes the reactivity trends among TMOs, and
would initiate viable design principles for, but not limited to, OER
catalysts
In Situ Spectroscopic Identification of μ‑OO Bridging on Spinel Co<sub>3</sub>O<sub>4</sub> Water Oxidation Electrocatalyst
The formation of ÎĽ-OO peroxide
(Co–OO–Co) moieties
on spinel
Co<sub>3</sub>O<sub>4</sub> electrocatalyst prior to the rise of the
electrochemical oxygen evolution reaction (OER) current was identified
by in situ spectroscopic methods. Through a combination of independent
in situ X-ray absorption, grazing-angle X-ray diffraction, and Raman
analysis, we observed a clear coincidence between the formation of
ÎĽ-OO peroxide moieties and the rise of the anodic peak during
OER. This finding implies that a chemical reaction step could be generally
ignored before the onset of OER current. More importantly, the tetrahedral
Co<sup>2+</sup> ions in the spinel Co<sub>3</sub>O<sub>4</sub> could
be the vital species to initiate the formation of the ÎĽ-OO peroxide
moieties
Sulfur-Mediated Self-Templating Synthesis of Tapered C‑PAN/g‑C<sub>3</sub>N<sub>4</sub> Composite Nanotubes toward Efficient Photocatalytic H<sub>2</sub> Evolution
Hollow one-dimensional
(1-D) nanostructures have drawn great attention
in heterogeneous photocatalysis. Herein, we report that tapered polyacrylonitrile-derived
carbon (C-PAN)/g-C<sub>3</sub>N<sub>4</sub> composite nanotubes can
be synthesized through a facile sulfur-mediated self-templating method
via thermal condensation of polyacrylonitrile (PAN), melamine, and
sulfur. The hollow tapered C-PAN/g-C<sub>3</sub>N<sub>4</sub> composite
nanotubes exhibit superior photocatalytic H<sub>2</sub> evolution
performance under visible light irradiation. The 5 wt % C-PAN/g-C<sub>3</sub>N<sub>4</sub> composite nanotubes show a 16.7 times higher
photocatalytic H<sub>2</sub> evolution rate than that of pure g-C<sub>3</sub>N<sub>4</sub>, which is even 4.7 times higher than that of
a 5 wt % C-PAN/g-C<sub>3</sub>N<sub>4</sub> nanosheet composite obtained
without sulfur. The hollow nanotubular composite structure provides
g-C<sub>3</sub>N<sub>4</sub> with higher specific surface area, enhanced
light absorption, and better charge carrier separation and transfer,
which synergistically contribute to the superior photocatalytic activity.
Our work provides a new strategy to develop carbon-based architected
photocatalysts