7 research outputs found
Lithium Niobate-Type Oxides as Visible Light Photovoltaic Materials
Lithium Niobate-Type Oxides as Visible Light Photovoltaic Material
Ferroelectric Oxides with Strong Visible-Light Absorption from Charge Ordering
The
applications of transition metal oxides as photovoltaic and
photocatalytic materials are mainly impeded by their poor visible
light absorption, low photogenerated carrier mobility, and low valence
band position, which originate from the generally large band gap (ā„3
eV), narrow transition metal <i>d</i> states, and deep oxygen
2<i>p</i> states. Here, we conceive a design strategy to
realize small band gap polar oxides with high carrier mobilities by
combining small radii <i>A</i> cations with Bi<sup>3+</sup>/Bi<sup>5+</sup> charge disproportion. We show that these cation
sizes and chemical features shift the valence band edge to higher
energies and therefore reduce the band gap, promoting the formation
of highly dispersive Bi 6<i>s</i> states near the Fermi
level as a byproduct. By means of advanced many-electron-based first-principles
calculations, we predict a new family of thermodynamically stable/metastable
polar oxides <i>A</i>BiO<sub>3</sub> (<i>A</i> = Ca, Cd, Zn, and Mg), which adopt the Ni<sub>3</sub>TeO<sub>6</sub>-type (space group <i>R</i>3) structure and exhibit optical
band gaps of ā¼2.0 eV, as promising single phase photovoltaic
and photocatalytic materials operating in the visible light spectrum
Experimental and Ab-Initio Investigation of the Electrical Conductivity of Emeraldine Salt
We present an experimental and first-principles
study to describe
the changes in the electrical conductivity properties of the Emeraldine
Salt (ES) form of polyaniline when using two different synthesis methods.
The ES powders obtained by the interfacial synthesis method (PANI-I)
exhibit higher electrical conductivity than that of the powders obtained
by the conventional method (PANI-C). Investigation of the calculated
band structure and density of states together with experimentally
obtained optical-absorption spectra and the magnetic measurements
indicate that PANI-I differs from PANI-C with respect to its localized
defect state type which significantly alters the intrinsic conductivity.
Furthermore, comparative studies of bond length, dihedral angles,
and relative stabilities of Leucomeraldine Base, Emeraldine Base,
ES Bipolaron state (ESB), and Polaron state (ESP) indicate that ESB
and ESP states might coexist. Additionally, we confirm that increasing
the length of the polymer chain to octamer in the unit cell does not
influence the relative stability between ESB and ESP defect states
Halogen-Induced Corrosion of Platinum
Halogen-Induced Corrosion of Platinu
Water Adsorption at the Tetrahedral Titania Surface Layer of SrTiO<sub>3</sub>(110)-(4 Ć 1)
The
interaction of water with oxide surfaces is of great interest
for both fundamental science and applications. We present a combined
theoretical (density functional theory (DFT)) and experimental (scanning
tunneling microscopy (STM) and photoemission spectroscopy (PES)) study
of water interaction with the two-dimensional titania overlayer that
terminates the SrTiO<sub>3</sub>(110)-(4 Ć 1) surface and consists
of TiO<sub>4</sub> tetrahedra. STM and core-level and valence band
PES show that H<sub>2</sub>O neither adsorbs nor dissociates on the
stoichiometric surface at room temperature, whereas it does dissociate
at oxygen vacancies. This is in agreement with DFT calculations, which
show that the energy barriers for water dissociation on the stoichiometric
and reduced surfaces are 1.7 and 0.9 eV, respectively. We propose
that water weakly adsorbs on two-dimensional, tetrahedrally coordinated
overlayers
A Multitechnique Study of C<sub>2</sub>H<sub>4</sub> Adsorption on Fe<sub>3</sub>O<sub>4</sub>(001)
The adsorption/desorption
of ethene (C2H4), also commonly known as ethylene,
on Fe3O4(001) was studied under ultrahigh vacuum
conditions using temperature-programmed
desorption (TPD), scanning tunneling microscopy, X-ray photoelectron
spectroscopy, and density functional theory (DFT)-based computations.
To interpret the TPD data, we have employed a new analysis method
based on equilibrium thermodynamics. C2H4 adsorbs
intact at all coverages and interacts most strongly with surface defects
such as antiphase domain boundaries and Fe adatoms. On the regular
surface, C2H4 binds atop surface Fe sites up
to a coverage of 2 molecules per (ā2 Ć ā2)R45Ā°
unit cell, with every second Fe occupied. A desorption energy of 0.36
eV is determined by analysis of the TPD spectra at this coverage,
which is approximately 0.1ā0.2 eV lower than the value calculated
by DFT + U with van der Waals corrections. Additional molecules are
accommodated in between the Fe rows. These are stabilized by attractive
interactions with the molecules adsorbed at Fe sites. The total capacity
of the surface for C2H4 adsorption is found
to be close to 4 molecules per (ā2 Ć ā2)R45Ā°
unit cell
Behavior of Methylammonium Dipoles in MAPbX<sub>3</sub> (X = Br and I)
Dielectric
constants of MAPbX<sub>3</sub> (X = Br, I) in the 1
kHzā1 MHz range show strong temperature dependence near room
temperature, in contrast to the nearly temperature-independent dielectric
constant of CsPbBr<sub>3</sub>. This strong temperature dependence
for MAPbX<sub>3</sub> in the tetragonal phase is attributed to the
MA<sup>+</sup> dipoles rotating freely within the probing time scale.
This interpretation is supported by ab initio molecular dynamics simulations
on MAPbI<sub>3</sub> that establish these dipoles as randomly oriented
with a rotational relaxation time scale of ā¼7 ps at 300 K.
Further, we probe the intriguing possibility of transient polarization
of these dipoles following a photoexcitation process with important
consequences on the photovoltaic efficiency, using a photoexcitation
pump and second harmonic generation efficiency as a probe with delay
times spanning 100 fsā1.8 ns. The absence of a second harmonic
signal at any delay time rules out the possibility of any transient
ferroelectric state under photoexcitation