50 research outputs found
Graphite and Hexagonal Boron-Nitride have the Same Interlayer Distance. Why?
Graphite and hexagonal boron nitride (<i>h</i>-BN) are
two prominent members of the family of layered materials possessing
a hexagonal lattice structure. While graphite has nonpolar homonuclear
C–C intralayer bonds, <i>h</i>-BN presents highly
polar B–N bonds resulting in different optimal stacking modes
of the two materials in the bulk form. Furthermore, the static polarizabilities
of the constituent atoms considerably differ from each other, suggesting
large differences in the dispersive component of the interlayer bonding.
Despite these major differences, both materials present practically
identical interlayer distances. To understand this finding, a comparative
study of the nature of the interlayer bonding in both materials is
presented. A full lattice sum of the interactions between the partially
charged atomic centers in <i>h</i>-BN results in vanishingly
small contributions to the interlayer binding energy. Higher order
electrostatic multipoles, exchange, and short-range correlation Kohn–Sham
contributions are found to be very similar in both materials and to
almost completely cancel out by the kinetic energy term, which partly
represents the effects of Pauli repulsions, at physically relevant
interlayer distances, resulting in a marginal effective contribution
to the interlayer binding. Further analysis of the dispersive energy
term reveals that despite the large differences in the individual
atomic polarizabilities, the heteroatomic B–N C<sub>6</sub> coefficient is very similar to the homoatomic C–C coefficient
in the hexagonal bulk form, resulting in very similar dispersive contribution
to the interlayer binding. The overall binding energy curves of both
materials are thus very similar, predicting practically the same interlayer
distance and very similar binding energies. The conclusions drawn
here regarding the role of electrostatic interactions between partially
charged atomic centers for the interlayer binding of <i>h</i>-BN are of a general nature and are expected to hold true for many
other polar layered systems
Controlling the Electronic Properties of Nanodiamonds via Surface Chemical Functionalization: A DFT Study
The electronic properties of chemically
functionalized nanodiamonds
are studied using density functional theory calculations. HOMO–LUMO
gaps and relative stabilities are calculated for different surface
functionalization schemes and diamond nanocrystal morphologies. The
effects of chemical decoration on the size and nature of the HOMO–LUMO
gap of the various systems considered are discussed in detail. We
conclude that surface chemical functionalization has the potential
to become an accessible route for controlling the electronic properties
of nanodiamonds
Controlling the Electronic Properties of Nanodiamonds via Surface Chemical Functionalization: A DFT Study
The electronic properties of chemically
functionalized nanodiamonds
are studied using density functional theory calculations. HOMO–LUMO
gaps and relative stabilities are calculated for different surface
functionalization schemes and diamond nanocrystal morphologies. The
effects of chemical decoration on the size and nature of the HOMO–LUMO
gap of the various systems considered are discussed in detail. We
conclude that surface chemical functionalization has the potential
to become an accessible route for controlling the electronic properties
of nanodiamonds
Effects of Edge Oxidation on the Structural, Electronic, and Magnetic Properties of Zigzag Boron Nitride Nanoribbons
The effects of edge chemistry on
the relative stability and electronic
properties of zigzag boron nitride nanoribbons (ZBNNRs) are investigated.
Among all functional groups considered, fully hydroxylated ZBNNRs
are found to be the most energetically stable. When an in-plane external
electric field is applied perpendicular to the axis of both hydrogenated
and hydroxylated ZBNNRs, a spin-polarized half-metallic state is induced,
whose character is different than that predicted for zigzag graphene
nanoribbons. The onset field for achieving the half-metallic state
is found to mainly depend on the width of the ribbon. Our results
indicate that edge functionalization of ZBNNRs may open the way for
the design of new nanoelectronic and nanospintronic devices
Registry-Dependent Peeling of Layered Material Interfaces: The Case of Graphene Nanoribbons on Hexagonal Boron Nitride
Peeling of layered materials from
supporting substrates, which
is central for exfoliation and transfer processes, is found to be
dominated by lattice commensurability effects in both low and high
velocity limits. For a graphene nanoribbon atop a hexagonal boron
nitride surface, the microscopic peeling behavior ranges from stick-slip,
through smooth-sliding, to pure peeling regimes, depending on the
relative orientation of the contacting surfaces and the peeling angle.
The underlying mechanisms stem from the intimate relation between
interfacial registry, interlayer interactions, and friction. This,
in turn, allows for devising simple models for extracting the interfacial
adhesion energy from the peeling force traces
Registry-Dependent Peeling of Layered Material Interfaces: The Case of Graphene Nanoribbons on Hexagonal Boron Nitride
Peeling of layered materials from
supporting substrates, which
is central for exfoliation and transfer processes, is found to be
dominated by lattice commensurability effects in both low and high
velocity limits. For a graphene nanoribbon atop a hexagonal boron
nitride surface, the microscopic peeling behavior ranges from stick-slip,
through smooth-sliding, to pure peeling regimes, depending on the
relative orientation of the contacting surfaces and the peeling angle.
The underlying mechanisms stem from the intimate relation between
interfacial registry, interlayer interactions, and friction. This,
in turn, allows for devising simple models for extracting the interfacial
adhesion energy from the peeling force traces
Numerical Approach to Nonequilibrium Quantum Thermodynamics: Nonperturbative Treatment of the Driven Resonant Level Model Based on the Driven Liouville von-Neumann Formalism
Nonequilibrium thermodynamics of
the driven resonant-level model
is studied using numerical simulations based on the driven Liouville
von-Neumann formalism. The approach is first validated against recently
obtained analytical results for quasistatic level shifts and the corresponding
first-order corrections. The numerical approach is then used to study
far-from-equilibrium thermodynamic properties of the system under
finite level shift rates. The proposed methodology allows the study
of unexplored nonequilibrium thermodynamic regimes in open quantum
systems
Registry-Dependent Peeling of Layered Material Interfaces: The Case of Graphene Nanoribbons on Hexagonal Boron Nitride
Peeling of layered materials from
supporting substrates, which
is central for exfoliation and transfer processes, is found to be
dominated by lattice commensurability effects in both low and high
velocity limits. For a graphene nanoribbon atop a hexagonal boron
nitride surface, the microscopic peeling behavior ranges from stick-slip,
through smooth-sliding, to pure peeling regimes, depending on the
relative orientation of the contacting surfaces and the peeling angle.
The underlying mechanisms stem from the intimate relation between
interfacial registry, interlayer interactions, and friction. This,
in turn, allows for devising simple models for extracting the interfacial
adhesion energy from the peeling force traces
Nanotube Slidetronics
One-dimensional slidetronics
is predicted for double-walled boron-nitride
nanotubes. Local electrostatic polarization patterns along the body
of the nanotube are found to be determined by the nature of the two
nanotube walls, their relative configuration, and circumferential
faceting modulation during coaxial interwall sliding. By careful choice
of chiral indices, chiral polarization patterns can emerge that spiral
around the nanotube circumference. The potential usage of the discovered
slidetronic effect for low-dimensional nanogenerators is briefly discussed
