73 research outputs found
Valence Band Splitting on Multilayer MoS<sub>2</sub>: Mixing of Spin–Orbit Coupling and Interlayer Coupling
Understanding the origin of valence
band splitting is important
because it governs the unique spin and valley physics in few-layer
MoS<sub>2</sub>. We explore the effects of spin–orbit coupling
and interlayer coupling on few-layer MoS<sub>2</sub> using first-principles
methods. We find spin–orbit coupling has a major contribution
to the valence band splitting at K in multilayer MoS<sub>2</sub>.
In double-layer MoS<sub>2</sub>, the interlayer coupling leads to
the widening of the gap between the already spin–orbit split
states. This is also the case for the bands of the K-point in bulk
MoS<sub>2</sub>. In triple-layer MoS<sub>2</sub>, the strength of
interlayer coupling of the spin-up channel becomes different from
that of spin-down at K. This combined with spin–orbit coupling
results in the band splitting in two main valence bands at K. With
the increase of pressure, this phenomenon becomes more obvious with
a decrease of main energy gap in the splitting valence bands at the
K valley
Nitrogen/Boron Doping Position Dependence of the Electronic Properties of a Triangular Graphene
We investigate the effect of N/B doping on the electronic properties for a zero-dimensional zigzag-edged triangular graphene, wherein two sets of sublattices are unbalanced, using density functional theory (DFT). We find that the substitutional N/B atom energetically prefers to distribute in the major sublattice. After the N/B doping, the net spin for triangular graphene is reduced and full or partial depolarization occurs depending on doping sites. Our DFT calculations show that the triangular graphene with N/B doped in the major sublattice has a larger energy gap, and the electronic properties depend on the doping position. There is an impurity state below or above the Fermi level for the N/B-doped triangular graphene, depending on the sublattice at which the dopant locates. The dependence of the electronic properties on doping position is attributed to the competition between the Coulomb attraction of N+ (B−) and the correlation with nonbonding states for the extra charge introduced by the N/B atom
Calculated band structure of cubic BaSnO<sub>3</sub> using the TB-mBJ potential.
<p>Calculated band structure of cubic BaSnO<sub>3</sub> using the TB-mBJ potential.</p
Calculated conduction band structure of the relaxed (KTaO<sub>3</sub>)//(CaSnO<sub>3</sub>) supercell (see text) using the TB-mBJ potential.
<p>The Fermi energy is at 0 eV. Spin orbit is included.</p
Calculated band gap of BaSnO<sub>3</sub> as a function of lattice parameter with the TB-mBJ potential.
<p>Calculated band gap of BaSnO<sub>3</sub> as a function of lattice parameter with the TB-mBJ potential.</p
Modulation of Hydrogen Evolution Catalytic Activity of Basal Plane in Monolayer Platinum and Palladium Dichalcogenides
With an appropriate
catalyst, hydrogen evolution reaction (HER)
by water splitting can be used to produce hydrogen gas. Recently,
layered transition-metal dichalcogenides have been proposed as alternative
HER catalysts. However, a significant challenge is how to obtain the
high-density active sites. With first-principle calculations, we explore
the possibility of defect engineering to trigger the HER catalytic
activity of basal plane by analyzing monolayer PdSe2, PtSe2, PdTe2, and PtTe2. It is found that
the double-vacancy DVSe (DVTe) and B-doping
can modulate appropriately the interaction between H and basal plane
and improve the HER activity of these transition-metal dichalcogenides.
Especially, the B-doping with high concentration can increase enormously
the density of active sites on basal plane
Highly Ordered Periodic Au/TiO<sub>2</sub> Hetero-Nanostructures for Plasmon-Induced Enhancement of the Activity and Stability for Ethanol Electro-oxidation
The
catalytic electro-oxidation of ethanol is the essential technique
for direct alcohol fuel cells (DAFCs) in the area of alternative energy
for the ability of converting the chemical energy of alcohol into
the electric energy directly. Developing highly efficient and stable
electrode materials with antipoisoning ability for ethanol electro-oxidation
remains a challenge. A highly ordered periodic Au-nanoparticle (NP)-decorated
bilayer TiO<sub>2</sub> nanotube (BTNT) heteronanostructure was fabricated
by a two-step anodic oxidation of Ti foil and the subsequent photoreduction
of HAuCl<sub>4</sub>. The plasmon-induced charge separation on the
heterointerface of Au/TiO<sub>2</sub> electrode enhances the electrocatalytic
activity and stability for the ethanol oxidation under visible light
irradiation. The highly ordered periodic heterostructure on the electrode
surface enhanced the light harvesting and led to the greater performance
of ethanol electro-oxidation under irradiation compared with the ordinary
Au NPs-decorated monolayer TiO<sub>2</sub> nanotube (MTNT). This novel
Au/TiO<sub>2</sub> electrode also performed a self-cleaning property
under visible light attributed to the enhanced electro-oxidation of
the adsorbed intermediates. This light-driven enhancement of the electrochemical
performances provides a development strategy for the design and construction
of DAFCs
Calculated conduction band structure of the relaxed (KNbO<sub>3</sub>)//(ZnSnO<sub>3</sub>) supercell (see text) using the TB-mBJ potential.
<p>The Fermi energy is at 0 eV.</p
Structures of supercells, left to right (a) KNbO<sub>3</sub>//CaSnO<sub>3</sub>, (b) KNbO<sub>3</sub>//ZnSnO<sub>3</sub>, (c) KTaO<sub>3</sub>//CaSnO<sub>3</sub>, and (d) KTaO<sub>3</sub>//ZnSnO<sub>3</sub>.
<p>As seen, the structures containing ZnSnO<sub>3</sub> have noticeable cation offcentering in the coordinating O cages in both the ZnSnO<sub>3</sub> and K(Nb,Ta)O<sub>3</sub> parts of the supercells. This corresponds to a ferroelectric polarization. The direction of this is indicated by the arrows on the left of the corresponding structure figures.</p
Calculated absorption spectrum of CaSnO<sub>3</sub> using the TB-mBJ potential.
<p>The Cartesian directions are along the crystallographic , and orthorhombic lattice parameters. A Lorentzian broadening of 0.025 eV was applied.</p
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