7 research outputs found
Topological Aspects of Charge-Carrier Transmission across Grain Boundaries in Graphene
Dislocations and grain boundaries
are intrinsic topological defects
of large-scale polycrystalline samples of graphene. These structural
irregularities have been shown to strongly affect electronic transport
in this material. Here, we report a systematic investigation of the
transmission of charge carriers across the grain-boundary defects
in polycrystalline graphene by means of the Landauer-Büttiker
formalism within the tight-binding approximation. Calculations reveal
a strong suppression of transmission at low energies upon decreasing
the density of dislocations with the smallest Burgers vector <b>b</b> = (1,0). The observed transport anomaly is explained from
the point of view of resonant backscattering due to localized states
of topological origin. These states are related to the gauge field
associated with all dislocations characterized by <b>b</b> =
(<i>n</i>,<i>m</i>) with <i>n</i> – <i>m</i> ≠
3<i>q</i> (<i>q</i> ∈ Z). Our work identifies an
important source of charge-carrier scattering caused by the topological
defects present in large-area graphene samples produced by chemical
vapor deposition
Chiral Decomposition of Twisted Graphene Multilayers with Arbitrary Stacking
We
formulate the chiral decomposition rules that govern the electronic
structure of a broad family of twisted N + M multilayer graphene configurations that combine arbitrary
stacking order and a mutual twist. We show that at the magic angle
in the chiral limit the low-energy bands of such systems are composed
of chiral pseudospin doublets that are energetically entangled with
two flat bands per valley induced by the moiré superlattice
potential. The analytic construction is supported by explicit numerical
calculations based on realistic parametrization. We further show that
vertical displacement fields can open energy gaps between the pseudospin
doublets and the two flat bands, such that the flat bands may carry
nonzero valley Chern numbers. These results provide guidelines for
the rational design of topological and correlated states in generic
twisted graphene multilayers
Grain Boundaries in Graphene on SiC(0001̅) Substrate
Grain boundaries in epitaxial graphene
on the SiC(0001̅)
substrate are studied using scanning tunneling microscopy and spectroscopy.
All investigated small-angle grain boundaries show pronounced out-of-plane
buckling induced by the strain fields of constituent dislocations.
The ensemble of observations determines the critical misorientation
angle of buckling transition θ<sub>c</sub> = 19 ± 2°.
Periodic structures are found among the flat large-angle grain boundaries.
In particular, the observed θ = 33 ± 2° highly ordered
grain boundary is assigned to the previously proposed lowest formation
energy structural motif composed of a continuous chain of edge-sharing
alternating pentagons and heptagons. This periodic grain boundary
defect is predicted to exhibit strong valley filtering of charge carriers
thus promising the practical realization of all-electric valleytronic
devices
Atomic Scale Microstructure and Properties of Se-Deficient Two-Dimensional MoSe<sub>2</sub>
We study the atomic scale microstructure of nonstoichiometric two-dimensional (2D) transition metal dichalcogenide MoSe<sub>2–<i>x</i></sub> by employing aberration-corrected high-resolution transmission electron microscopy. We show that a Se-deficit in single layers of MoSe<sub>2</sub> grown by molecular beam epitaxy gives rise to a dense network of mirror-twin-boundaries (MTBs) decorating the 2D-grains. With the use of density functional theory calculations, we further demonstrate that MTBs are thermodynamically stable structures in Se-deficient sheets. These line defects host spatially localized states with energies close to the valence band minimum, thus giving rise to enhanced conductance along straight MTBs. However, electronic transport calculations show that the transmission of hole charge carriers across MTBs is strongly suppressed due to band bending effects. We further observe formation of MTBs during <i>in situ</i> removal of Se atoms by the electron beam of the microscope, thus confirming that MTBs appear due to Se-deficit, and not coalescence of individual grains during growth. At a very high local Se-deficit, the 2D sheet becomes unstable and transforms to a nanowire. Our results on Se-deficient MoSe<sub>2</sub> suggest routes toward engineering the properties of 2D transition metal dichalcogenides by deviations from the stoichiometric composition
Atomic Scale Microstructure and Properties of Se-Deficient Two-Dimensional MoSe<sub>2</sub>
We study the atomic scale microstructure of nonstoichiometric two-dimensional (2D) transition metal dichalcogenide MoSe<sub>2–<i>x</i></sub> by employing aberration-corrected high-resolution transmission electron microscopy. We show that a Se-deficit in single layers of MoSe<sub>2</sub> grown by molecular beam epitaxy gives rise to a dense network of mirror-twin-boundaries (MTBs) decorating the 2D-grains. With the use of density functional theory calculations, we further demonstrate that MTBs are thermodynamically stable structures in Se-deficient sheets. These line defects host spatially localized states with energies close to the valence band minimum, thus giving rise to enhanced conductance along straight MTBs. However, electronic transport calculations show that the transmission of hole charge carriers across MTBs is strongly suppressed due to band bending effects. We further observe formation of MTBs during <i>in situ</i> removal of Se atoms by the electron beam of the microscope, thus confirming that MTBs appear due to Se-deficit, and not coalescence of individual grains during growth. At a very high local Se-deficit, the 2D sheet becomes unstable and transforms to a nanowire. Our results on Se-deficient MoSe<sub>2</sub> suggest routes toward engineering the properties of 2D transition metal dichalcogenides by deviations from the stoichiometric composition
Creating Law at the Securities and Exchange Commission: The Lawyer as Prosecutor
Transition
metal dichalcogenides (TMDCs), together with other two-dimensional
(2D) materials, have attracted great interest due to the unique optical
and electrical properties of atomically thin layers. In order to fulfill
their potential, developing large-area growth and understanding the
properties of TMDCs have become crucial. Here, we have used molecular
beam epitaxy (MBE) to grow atomically thin MoSe<sub>2</sub> on GaAs(111)B.
No intermediate compounds were detected at the interface of as-grown
films. Careful optimization of the growth temperature can result in
the growth of highly aligned films with only two possible crystalline
orientations due to broken inversion symmetry. As-grown films can
be transferred onto insulating substrates, allowing their optical
and electrical properties to be probed. By using polymer electrolyte
gating, we have achieved ambipolar transport in MBE-grown MoSe<sub>2</sub>. The temperature-dependent transport characteristics can
be explained by the 2D variable-range hopping (2D-VRH) model, indicating
that the transport is strongly limited by the disorder in the film
Experimentally Engineering the Edge Termination of Graphene Nanoribbons
The edges of graphene nanoribbons (GNRs) have attracted much interest due to their potentially strong influence on GNR electronic and magnetic properties. Here we report the ability to engineer the microscopic edge termination of high-quality GNRs <i>via</i> hydrogen plasma etching. Using a combination of high-resolution scanning tunneling microscopy and first-principles calculations, we have determined the exact atomic structure of plasma-etched GNR edges and established the chemical nature of terminating functional groups for zigzag, armchair, and chiral edge orientations. We find that the edges of hydrogen-plasma-etched GNRs are generally flat, free of structural reconstructions, and terminated by hydrogen atoms with no rehybridization of the outermost carbon edge atoms. Both zigzag and chiral edges show the presence of edge states