6 research outputs found
Characteristics of Lithium Ions and Superoxide Anions in EMI-TFSI and Dimethyl Sulfoxide
To
clarify the microscopic effects of solvents on the formation
of the Li<sup>+</sup>-O<sub>2</sub><sup>–</sup> process of a Li–O<sub>2</sub> battery, we studied
the kinetics and thermodynamics of these ions in dimethyl sulfoxide
(DMSO) and 1-ethyl-3-methylimidazolium bisÂ(trifluoromethylsulfonyl)Âimide
(EMI-TFSI) using classical molecular dynamics simulation. The force
field for ions–solvents interactions was parametrized by force
matching first-principles calculations. Despite the solvation energies
of the ions are similar in both solvents, their mobility is much higher
in DMSO. The free-energy profiles also confirm that the formation
and decomposition rates of Li<sup>+</sup>-O<sub>2</sub><sup>–</sup> pairs are greater in DMSO than
in EMI-TFSI. Our atomistic simulations point out that the strong structuring
of EMI-TFSI around the ions is responsible for these differences,
and it explains why the LiO<sub>2</sub> clusters formed in DMSO during
the battery discharge are larger than those in EMI-TFSI. Understanding
the origin of such properties is crucial to aid the optimization of
electrolytes for Li–O<sub>2</sub> batteries
Imaging the Evolution of <i>d</i> States at a Strontium Titanate Surface
Oxide electronics
is a promising alternative to the conventional
silicon-based semiconductor technology, owing to the rich functionalities
of oxide thin films and heterostructures. In contrast to the silicon
surface, however, the electronic structure of the SrTiO<sub>3</sub> surface, the most important substrate for oxide thin films growth,
is not yet completely understood. Here we report on the electronic
states of a reconstructed (001) surface of SrTiO<sub>3</sub> determined
in real space, with scanning tunneling microscopy/spectroscopy and
density functional theory calculations. We found a remarkable energy
dependence of the spectroscopic image: Theoretical analysis reveals
that symmetry breaking at the surface lifts the degeneracy in the <i>t</i><sub>2<i>g</i></sub> state (<i>d</i><sub><i>xy</i></sub>, <i>d</i><sub><i>yz</i></sub>, and <i>d</i><sub><i>zx</i></sub>) of
Ti 3<i>d</i> orbitals, whose anisotropic spatial distribution
leads to a sharp transition in the spectroscopic image as a function
of energy. The knowledge obtained here could be used to gain further
insights into emergent phenomena at the surfaces and interfaces with
SrTiO<sub>3</sub>
Self-Assembly Strategy for Fabricating Connected Graphene Nanoribbons
We use self-assembly to fabricate and to connect precise graphene nanoribbons end to end. Combining scanning tunneling microscopy, Raman spectroscopy, and density functional theory, we characterize the chemical and electronic aspects of the interconnections between ribbons. We demonstrate how the substrate effects of our self-assembly can be exploited to fabricate graphene structures connected to desired electrodes
Electronic Structure and Photoelectrochemical Properties of an Ir-Doped SrTiO<sub>3</sub> Photocatalyst
The
effect of iridium valence in Ir:SrTiO<sub>3</sub> on the electronic
structure and the photocatalytic activity in a water splitting reaction
was studied. Epitaxial thin film photoelectrodes were grown with controlled
Ir valence and used to measure the electrochemical efficiency of Ir:SrTiO<sub>3</sub>. The positions of the in-gap Ir impurity levels were determined
by optical and X-ray photoelectron spectroscopies. Comparison with
ab initio calculations was used to assign the observed electronic
states to either Ir<sup>4+</sup> or Ir<sup>3+</sup> dopants in SrTiO<sub>3</sub>. The measurements show that Ir<sup>3+</sup>:SrTiO<sub>3</sub> forms a single midgap impurity state that is strongly localized,
completely quenching the photoelectrochemical response. An anodic
photoresponse was seen in Ir<sup>4+</sup>:SrTiO<sub>3</sub> under
visible-light illumination up to a wavelength of 600 nm (hν
= 2.0 eV). Ir<sup>4+</sup>:SrTiO<sub>3</sub> contains an in-gap state
close to the top of the SrTiO<sub>3</sub> valence band. The performance
of Ir<sup>4+</sup>:SrTiO<sub>3</sub> in electrochemical reactions
is compared with cathodic Rh<sup>3+</sup>:SrTiO<sub>3</sub>, clearly
illustrating the importance of strong dopant d-electron hybridization
with the oxygen 2p valence band of SrTiO<sub>3</sub> for improving
the energy conversion efficiency in SrTiO<sub>3</sub>-based photocatalysts
Bottom-Up Graphene-Nanoribbon Fabrication Reveals Chiral Edges and Enantioselectivity
We produce precise chiral-edge graphene nanoribbons on Cu{111} using self-assembly and surface-directed chemical reactions. We show that, using specific properties of the substrate, we can change the edge conformation of the nanoribbons, segregate their adsorption chiralities, and restrict their growth directions at low surface coverage. By elucidating the molecular-assembly mechanism, we demonstrate that our method constitutes an alternative bottom-up strategy toward synthesizing defect-free zigzag-edge graphene nanoribbons
Elucidation of Rh-Induced In-Gap States of Rh:SrTiO<sub>3</sub> Visible-Light-Driven Photocatalyst by Soft X‑ray Spectroscopy and First-Principles Calculations
The occupied and unoccupied in-gap electronic states
of a Rh-doped
SrTiO<sub>3</sub> photocatalyst were investigated by X-ray emission
spectroscopy and X-ray absorption spectroscopy for different Rh impurity
valence states and doping levels. An unoccupied midgap Rh<sup>4+</sup> acceptor state was found 1.5 eV below the SrTiO<sub>3</sub> conduction
band minimum. Both Rh<sup>4+</sup> and Rh<sup>3+</sup> dopants were
found to have an occupied donor level close to the valence band maximum
of SrTiO<sub>3</sub>. The density of states obtained from first-principles
calculations show that all observed spectral features can be assigned
to electronic states of substitutional Rh at the Ti site and that
Rh:SrTiO<sub>3</sub> is an unusual titanate compound with a characteristic
p-type electronic structure. The Rh doping results in a large decrease
of the bandgap energy, making Rh:SrTiO<sub>3</sub> an attractive material
for use as a visible-light-driven H<sub>2</sub>-evolving photocatalyst
in a solar water splitting reaction