3 research outputs found
Healing Se Vacancies in Bi<sub>2</sub>Se<sub>3</sub> by Ambient Gases
Selenium
(Se) vacancies are the most abundant and unavoidable n-type
defects in the topological insulator, bismuth selenide (Bi2Se3). A recent study has shown that the surface Se vacancies
not only n-dope the system but also result in the
splitting of the Dirac cone associated with the surface and the emergence
of a nonlinear state pinned at the Fermi level due to the interactions
between surface-, defect-, and quantum-well states. In this combined
theoretical and experimental work, we show how the defective surfaces
of Bi2Se3 slabs can be healed by adsorption
of different gases. Depending on the adsorbates, we find that the
band structure of Bi2Se3 either reverts back
to its pristine form or exhibits localized adsorbate bands near the
Fermi level. Notably, our density functional theory calculations show
that both atomic and molecular oxygen are isoelectronic to Se, binding
strongly to the vacancy position. Along with counterdoping (p-doping)
of Bi2Se3 (as reported by earlier studies),
oxygen adsorption completely restores the Dirac structure of the surface
states. Our experiments confirm that annealing intrinsically n-doped Bi2Se3 samples with oxygen
reduces the carrier density by ≈ 6%. This is a reversible process,
with the Bi2Se3 slab reverting back to the original
carrier concentration on vacuum annealing, thus confirming the healing
of vacancies by oxygen. We distinguish the possible features of the
adsorbates that can be used to a priori predict their effects on the
electronic structure of the Bi2Se3 slab after
adsorption. Our results provide a foundation for a general strategy
for the in situ engineering of the band structure of the Bi2Se3 family of topological insulators by quenching Se vacancies
van der Waals Screening by Single-Layer Graphene and Molybdenum Disulfide
A sharp tip of atomic force microscope is employed to probe van der Waals forces of a silicon oxide substrate with adhered graphene. Experimental results obtained in the range of distances from 3 to 20 nm indicate that single-, double-, and triple-layer graphenes screen the van der Waals forces of the substrate. Fluorination of graphene, which makes it electrically insulating, lifts the screening in the single-layer graphene. The van der Waals force from graphene determined per layer decreases with the number of layers. In addition, increased hole doping of graphene increases the force. Finally, we also demonstrate screening of the van der Waals forces of the silicon oxide substrate by single- and double-layer molybdenum disulfide
Nitrogen-Doped Graphene and Twisted Bilayer Graphene <i>via</i> Hyperthermal Ion Implantation with Depth Control
We investigate hyperthermal ion implantation
(HyTII) as a means
for substitutionally doping layered materials such as graphene. In
particular, this systematic study characterizes the efficacy of substitutional
N-doping of graphene using HyTII over an N<sup>+</sup> energy range
of 25–100 eV. Scanning tunneling microscopy results establish
the incorporation of N substituents into the graphene lattice during
HyTII processing. We illustrate the differences in evolution of the
characteristic Raman peaks following incremental doses of N<sup>+</sup>. We use the ratios of the integrated D and D′ peaks, <i>I</i>(D)/<i>I</i>(D′) to assess the N<sup>+</sup> energy-dependent doping efficacy, which shows a strong correlation
with previously reported molecular dynamics (MD) simulation results
and a peak doping efficiency regime ranging between approximately
30 and 50 eV. We also demonstrate the inherent monolayer depth control
of the HyTII process, thereby establishing a unique advantage over
other less-specific methods for doping. We achieve this by implementing
twisted bilayer graphene (TBG), with one layer of isotopically enriched <sup>13</sup>C and one layer of natural <sup>12</sup>C graphene, and modify
only the top layer of the TBG sample. By assessing the effects of
N-HyTII processing, we uncover dose-dependent shifts in the transfer
characteristics consistent with electron doping and we find dose-dependent
electronic localization that manifests in low-temperature magnetotransport
measurements