30 research outputs found
Surface Structure and Reactivity of Anatase TiO<sub>2</sub> Crystals with Dominant {001} Facets
Hydrofluoric acid (HF)-assisted hydrothermal/solvothermal
methods
are widely used to synthesize anatase TiO<sub>2</sub> single crystals
with a high percentage of {001} facets, which are generally considered
to be highly reactive. We have used Density Functional Theory calculations
and first principles molecular dynamics simulations to investigate
the structure of these facets, which is not yet well understood. Our
results suggest that (001) surfaces exhibit the bulk-terminated structure
when in contact with concentrated HF solutions. However, (1 Ă—
4)-reconstructed surfaces, as observed in UHV, become always more
stable at the typical temperatures, 400–600 °C, used to
clean the as-prepared crystals in experiments. Since the (1 Ă—
4)-reconstructed surfaces are only weakly reactive, our results predict
that synthetic anatase crystals with dominant {001} facets should
not exhibit enhanced photocatalytic activity, consistent with recent
experimental observations
Water Adsorption and Oxidation at the Co<sub>3</sub>O<sub>4</sub> (110) Surface
We carried
out density functional theory calculations with on-site Coulomb repulsion
U terms to study the interaction of water with the (110) surface of
the spinel cobalt oxide, Co<sub>3</sub>O<sub>4</sub>, a widely used
oxidation catalyst. This surface has two different terminations, one
positively (A) and the other negatively charged (B). Dissociative
water adsorption is preferred from low up to one monolayer coverage
on the A termination and up to half monolayer on the B termination.
On the latter, a mixed molecular and dissociated monolayer is more
stable at full coverage. The computed structures are used to investigate
the free-energy changes during water oxidation on both surface terminations.
We find that the most difficult step of the oxygen evolution reaction
is the second deprotonation to form an adsorbed O species (O*). Moreover,
the A-terminated surface is more active than the B-terminated surface.
Analysis of the surface electronic structure shows a larger density
of cobalt states near the Fermi energy on the A termination, which
stabilizes the O* species and thus reduces the overpotential
Mosaic Texture and Double <i>c</i>‑Axis Periodicity of β‑NiOOH: Insights from First-Principles and Genetic Algorithm Calculations
Fe-doped NiO<sub><i>x</i></sub> has recently emerged
as a promising anode material for the oxygen evolution reaction, but
the origin of the high activity is still unclear, due largely to the
structural uncertainty of the active phase of NiO<sub><i>x</i></sub>. Here, we report a theoretical study of the structure of β-NiOOH,
one of the active components of NiO<sub><i>x</i></sub>.
Using a genetic algorithm search of crystal structures combined with
dispersion-corrected hybrid density functional theory calculations,
we identify two groups of favorable structures: (i) layered structures
with alternate NiÂ(OH)<sub>2</sub> and NiO<sub>2</sub> layers, consistent
with the doubling of the <i>c</i> axis observed in high
resolution transmission electron microscopy (TEM) measurements, and
(ii) tunnel structures isostructural with MnO<sub>2</sub> polymorphs,
which can provide a rationale for the mosaic textures observed in
TEM. Analysis of the Ni ions oxidation state further indicates a disproportionation
of half of the Ni<sup>3+</sup> cations to Ni<sup>2+</sup>/Ni<sup>4+</sup> pairs. Hybrid density functionals are found essential for a correct
description of the electronic structure of β-NiOOH
Theoretical Study of Interfacial Electron Transfer from Reduced Anatase TiO<sub>2</sub>(101) to Adsorbed O<sub>2</sub>
We study the electron transfer from
a reduced TiO<sub>2</sub> surface to an approaching O<sub>2</sub> molecule
using periodic hybrid density functional calculations. We find that
the formation of an adsorbed superoxo species, *O<sub>2</sub><sup>–</sup>, via the reaction O<sub>2</sub>(gas) + e<sup>–</sup> → *O<sub>2</sub><sup>–</sup>, is barrierless, whereas
the transfer of another electron to transform the superoxo into an
adsorbed peroxide, i.e. *O<sub>2</sub><sup>–</sup> + e<sup>–</sup> → *O<sub>2</sub><sup>2–</sup>, is nonadiabatic
and has a barrier of 0.3 eV. The origin of this nonadiabaticity is
attributed to the instability of an intermediate where the second
electron is localized at the superoxo adsorption site. These results
can explain the experimental finding that O<sub>2</sub> is not an
efficient electron scavenger in photocatalysis
Pathway of Photocatalytic Oxygen Evolution on Aqueous TiO<sub>2</sub> Anatase and Insights into the Different Activities of Anatase and Rutile
The
photocatalytic oxidation of water to molecular oxygen is a
key step toward the conversion of solar energy to fuels. Understanding
the detailed mechanism and kinetics of this reaction is important
for the development of robust catalysts with improved efficiency.
TiO<sub>2</sub> is one of the best-known photocatalysts as well as
a model system for the study of the oxygen evolution reaction (OER).
Here we use hybrid density functional based energetic calculations
and first-principles molecular dynamics simulations to investigate
the pathway and kinetics of the OER on the majority (101) surface
of anatase TiO<sub>2</sub> in a water environment. Our results show
that terminal Ti–OH groups are stable intermediates at the
aqueous (101) interface, in accord with the experimental observation
that OH radicals are efficiently produced on anatase. Oxidation of
Ti–OH gives rise to a second stable intermediate, a surface-bridging
peroxo dimer ((O<sub>2</sub><sup>2–</sup>)<sub>br</sub>) composed
of one water and one surface lattice oxygen atom, consistent with
the surface peroxo intermediates revealed by “in situ”
measurements on rutile. Our calculations further predict that molecular
oxygen evolves directly from (O<sub>2</sub><sup>2–</sup>)<sub>br</sub> through a concerted two-electron transfer, thus leading
to oxygen exchange between TiO<sub>2</sub> and the adsorbed species.
Oxygen exchange is found to be negligible on rutile, so that different
OER pathways are likely to be operative on the two main TiO<sub>2</sub> polymorphs. This difference could explain the observed lower OER
activity of anatase relative to rutile
Mechanism and Activity of Water Oxidation on Selected Surfaces of Pure and Fe-Doped NiO<sub><i>x</i></sub>
Mixed nickel–iron oxides have
recently emerged as promising
electrocatalysts for water oxidation because of their low cost and
high activity, but the composition and structure of the catalyst’s
active phase under working conditions are not yet fully established.
We present here density functional theory calculations with on-site
Coulomb repulsion of the energetics of the oxygen evolution reaction
(OER) on selected surfaces of pure and mixed Ni–Fe oxides that
are possible candidates for the catalyst’s active phase. The
investigated surfaces are pure β-NiOOH(011̅5) and γ-NiOOH(101),
Fe-doped β-NiOOH(011̅5) and γ-NiOOH(101), NiFe<sub>2</sub>O<sub>4</sub>(001), and Fe<sub>3</sub>O<sub>4</sub>(001).
We find that Fe-doped β-NiOOH(011̅5) has by far the lowest
overpotential (η = 0.26 V), followed by NiFe<sub>2</sub>O<sub>4</sub>(001) (η = 0.42 V). Our results indicate that Fe-doped
β-NiOOH and, to a lesser extent, NiFe<sub>2</sub>O<sub>4</sub> could be the phases responsible for the enhanced OER activity of
NiO<sub><i>x</i></sub> when it is doped with Fe
Bulk and Surface Polarons in Photoexcited Anatase TiO<sub>2</sub>
Using hybrid functional electronic structure calculations, we have investigated the structure and energetics of photogenerated electrons and holes in the bulk and at the (101) surface of anatase TiO<sub>2</sub>. Excitons formed upon UV irradiation are found to become self-trapped, consistent with the observation of temperature-dependent Urbach tails in the absorption spectrum and a large Stokes shift in the photoluminescence band of anatase. Electron and hole polarons are localized at Ti<sup>3+</sup> and O<sup>–</sup> lattice sites, respectively. At the surface, the trapping sites generally correspond to undercoordinated Ti<sup>3+</sup><sub>5c</sub> and O<sup>–</sup><sub>2c</sub> surface atoms or to isolated OH species in the case of a hydroxylated surface. The polaron trapping energy is considerably larger at the surface than in the bulk, indicating that it is energetically favorable for the polarons to travel from the bulk to the surface. Computed one-electron energy levels in the gap and hyperfine coupling constants compare favorably with oxidation potential and EPR measurements
Solvent Effects on the Adsorption Geometry and Electronic Structure of Dye-Sensitized TiO<sub>2</sub>: A First-Principles Investigation
The performance of dye-sensitized solar cells (DSSCs)
depends significantly
on the adsorption geometry of the dye on the semiconductor surface.
In turn, the stability and geometry of the adsorbed molecules is influenced
by the chemical environment at the electrolyte/dye/TiO<sub>2</sub> interface. To gain insight into the effect of the solvent on the
adsorption geometries and electronic properties of dye-sensitized
TiO<sub>2</sub> interfaces, we carried out first-principles calculations
on organic dyes and solvent (water or acetonitrile) molecules coadsorbed
on the (101) surface of anatase TiO<sub>2</sub>. Solvent molecules
introduce important modifications on the dye adsorption geometry with
respect to the geometry calculated in vacuo. In particular, the bonding
distance of the dye from the Ti anchoring atoms increases, the adsorption
energy decreases, and the two C–O bonds in the carboxylic moieties
become more symmetric than in vacuo. Moreover, the adsorbed solvent
induces the deprotonation of the dye due to the changing the acid/base
properties of the system. Analysis of the electronic structure for
the dye-sensitized TiO<sub>2</sub> structures in the presence of coadsorbed
solvent molecules shows an upward shift in the TiO<sub>2</sub> conduction
band of 0.2 to 0.5 eV (0.5 to 0.8 eV) in water (acetonitrile). A similar
shift is calculated for a solvent monolayer on unsensitized TiO<sub>2</sub>. The overall picture extracted from our calculations is consistent
with an upshift of the conduction band in acetonitrile (2.04 eV vs
SCE) relative to water (0.82 eV vs SCE, pH 7), as reported in previous
studies on TiO<sub>2</sub> flatband potential (Redmond, G.; Fitzmaurice,
D. <i>J. Phys. Chem.</i> <b>1993</b>, <i>97</i>, 1426–1430) and suggests a relevant role of the solvent in
determining the dye–semiconductor interaction and electronic
coupling
Ab Initio Simulation of the Absorption Spectra of Photoexcited Carriers in TiO<sub>2</sub> Nanoparticles
We
investigate the absorption spectra of photoexcited carriers
in a prototypical anatase TiO<sub>2</sub> nanoparticle using hybrid
time dependent density functional theory calculations in water solution.
Our results agree well with experimental transient absorption spectroscopy
data and shed light on the character of the transitions. The trapped
state is always involved, so that the SOMO/SUMO is the initial/final
state for the photoexcited electron/hole absorption. For a trapped
electron, final states in the low energy tail of the conduction band
correspond to optical transitions in the IR, while final states at
higher energy correspond to optical transitions in the visible. For
a trapped hole, the absorption band is slightly blue-shifted and narrower
in comparison to that of the electron, consistent with its deeper
energy level in the band gap. Our calculations also show that electrons
in shallow traps exhibit a broad absorption in the IR, resembling
the feature attributed to conductive electrons in experimental spectra
Formation, Electronic Structure, and Defects of Ni Substituted Spinel Cobalt Oxide: a DFT+U Study
Nickel
substituted spinel cobalt oxide is a promising technological
material with complex electronic and magnetic structures. Understanding
these structures is important for improving the material’s
performance in various applications. We have carried out first-principles
calculations on the formation, electronic properties, and defects
of bulk NiCo<sub>2</sub>O<sub>4</sub> using density functional theory
(DFT) with on-site Hubbard U terms on the transition metal d states.
Analysis of the electronic structure of Ni<sub><i>x</i></sub>Co<sub>3‑<i>x</i></sub>O<sub>4</sub> as a function
of <i>x</i> = 0–1 shows that Ni acts as a p-type
dopant in Co<sub>3</sub>O<sub>4</sub>, gradually transforming the
minority spin channel from insulating to conducting. As a result,
the inverse spinel NiCo<sub>2</sub>O<sub>4</sub> (NCO) is found to
have a ferrimagnetic half-metallic ground state with fractional valence
on Ni and Co cations at tetrahedral sites (Td), in agreement with
experimental observations. Projected densities of states confirm that
the states around the Fermi energy originate from Ni and CoÂ(Td) 3d
states hybridized with oxygen 2p orbitals. The influence of two common
defects, Ni ↔ CoÂ(Td) exchanges and oxygen vacancies, on the
structural and electronic properties has been also investigated. Our
results are consistent with the experimental observation that intermediate
structures between inverse spinel and normal spinel occur frequently
in NCO. Oxygen vacancies are predicted to occur more frequently at
sites coordinated to a larger number of Ni ions and found to have
only minor effects on the conductivity and magnetic structure