3 research outputs found
Tuning and Identification of Interband Transitions in Monolayer and Bilayer Molybdenum Disulfide Using Hydrostatic Pressure
Few-layer molybdenum disulfide (MoS<sub>2</sub>) is advantageous for application in next-generation electronic and optoÂelectronic devices. For monolayer MoS<sub>2</sub>, it has been established that both the conduction band minimum (CBM) and the valence band maximum (VBM) occur at the K point in the Brillouin zone. For bilayer MoS<sub>2</sub>, it is known that the VBM occurs at the Γ point. However, whether the K valley or the Λ valley forms the CBM and the energy difference between them remain disputable. Theoretical calculations have not provided a conclusive answer. In this paper, we demonstrate that a direct K–K to an indirect Λ–K interband transition in bilayer MoS<sub>2</sub> can be optically detected by tuning the hydrostatic pressure. A changeover of the CBM from the K valley to the Λ valley is observed to occur under a pressure of approximately 1.5 GPa. The experimental results clearly indicate that the K valley forms the CBM under zero strain, while the Λ valley is approximately 89 ± 9 meV higher in energy
Probing Spin–Orbit Coupling and Interlayer Coupling in Atomically Thin Molybdenum Disulfide Using Hydrostatic Pressure
In two-dimensional transition-metal
dichalcogenides, both spin–orbit
coupling and interlayer coupling play critical roles in the electronic
band structure and are desirable for the potential applications in
spin electronics. Here, we demonstrate the pressure characteristics
of the exciton absorption peaks (so-called excitons A, B and C) in
monolayer, bilayer, and trilayer molybdenum disulfide (MoS<sub>2</sub>) by studying the reflectance spectra under hydrostatic pressure
and performing the electronic band structure calculations based on
density functional theory to account for the experimental observations.
We find that the valence band maximum splitting at the K point in
monolayer MoS<sub>2</sub>, induced by spin–orbit coupling,
remains almost unchanged with increasing pressure applied up to 3.98
GPa, indicating that the spin–orbit coupling is insensitive
to the pressure. For bilayer and trilayer MoS<sub>2</sub>, however,
the splitting shows an increase with increasing pressure due to the
pressure-induced strengthening of the interlayer coupling. The experimental
results are in good agreement with the theoretical calculations. Moreover,
the exciton C is identified to be the interband transition related
to the van Hove singularity located at a special point which is approximately
1/4 of the total length of Γ–K away from the Γ
point in the Brillouin zone
Anomalous Pressure Characteristics of Defects in Hexagonal Boron Nitride Flakes
Research
on hexagonal boron nitride (hBN) has been intensified
recently due to the application of hBN as a promising system of single-photon
emitters. To date, the single photon origin remains under debate even
though many experiments and theoretical calculations have been performed.
We have measured the pressure-dependent photoluminescence (PL) spectra
of hBN flakes at low temperatures by using a diamond anvil cell device.
The absolute values of the pressure coefficients of discrete PL emission
lines are all below 15 meV/GPa, which is much lower than the pressure-induced
36 meV/GPa redshift rate of the hBN bandgap. These PL emission lines
originate from atom-like localized defect levels confined within the
bandgap of the hBN flakes. Interestingly, the experimental results
of the pressure-dependent PL emission lines present three different
types of pressure responses corresponding to a redshift (negative
pressure coefficient), a blueshift (positive pressure coefficient),
or even a sign change from negative to positive. Density functional
theory calculations indicate the existence of competition between
the intralayer and interlayer interaction contributions, which leads
to the different pressure-dependent behaviors of the PL peak shift