4 research outputs found
Tuning the Sharing Modes and Composition in a Tetrahedral GeX<sub>2</sub> (X = S, Se) System via One-Dimensional Confinement
The packing and connectivity of tetrahedral units are
central themes
in the structural and electronic properties of a host of solids. Here,
we report one-dimensional (1D) chains of GeX2 (X = S or
Se) with modification of the tetrahedral connectivity at the single-chain
limit. Precise tuning of the edge- and corner-sharing modes between
GeX2 blocks is achieved by diameter-dependent 1D confinement
inside a carbon nanotube. Atomic-resolution scanning transmission
electron microscopy directly confirms the existence of two distinct
types of GeX2 chains. Density functional theory calculations
corroborate the diameter-dependent stability of the system and reveal
an intriguing electronic structure that sensitively depends on tetrahedral
connectivity and composition. GeS2(1–x)Se2x compound chains are also
realized, which demonstrate the tunability of the system’s
semiconducting properties through composition engineering
In Situ Imaging of an Anisotropic Layer-by-Layer Phase Transition in Few-Layer MoTe<sub>2</sub>
Understanding the phase transition mechanisms in two-dimensional
(2D) materials is a key to precisely tailor their properties at the
nanoscale. Molybdenum ditelluride (MoTe2) exhibits multiple
phases at room temperature, making it a promising candidate for phase-change
applications. Here, we fabricate lateral 2H–Td interfaces with laser irradiation and probe
their phase transitions from micro- to atomic scales with in situ heating in the transmission electron microscope
(TEM). By encapsulating the MoTe2 with graphene protection
layers, we create an in situ reaction cell compatible
with atomic resolution imaging. We find that the Td-to-2H phase transition initiates at
phase boundaries at low temperatures (200–225 °C) and
propagates anisotropically along the b-axis in a
layer-by-layer fashion. We also demonstrate a fully reversible 2H-Td-2H phase
transition cycle, which generates a coherent 2H lattice
containing inversion domain boundaries. Our results provide insights
on fabricating 2D heterophase devices with atomically sharp and coherent
interfaces
In Situ Imaging of an Anisotropic Layer-by-Layer Phase Transition in Few-Layer MoTe<sub>2</sub>
Understanding the phase transition mechanisms in two-dimensional
(2D) materials is a key to precisely tailor their properties at the
nanoscale. Molybdenum ditelluride (MoTe2) exhibits multiple
phases at room temperature, making it a promising candidate for phase-change
applications. Here, we fabricate lateral 2H–Td interfaces with laser irradiation and probe
their phase transitions from micro- to atomic scales with in situ heating in the transmission electron microscope
(TEM). By encapsulating the MoTe2 with graphene protection
layers, we create an in situ reaction cell compatible
with atomic resolution imaging. We find that the Td-to-2H phase transition initiates at
phase boundaries at low temperatures (200–225 °C) and
propagates anisotropically along the b-axis in a
layer-by-layer fashion. We also demonstrate a fully reversible 2H-Td-2H phase
transition cycle, which generates a coherent 2H lattice
containing inversion domain boundaries. Our results provide insights
on fabricating 2D heterophase devices with atomically sharp and coherent
interfaces
Growth and Simultaneous Valleys Manipulation of Two-Dimensional MoSe<sub>2</sub>‑WSe<sub>2</sub> Lateral Heterostructure
The
covalently bonded in-plane heterostructure (HS) of monolayer
transition-metal dichalcogenides (TMDCs) possesses huge potential
for high-speed electronic devices in terms of valleytronics. In this
study, high-quality monolayer MoSe<sub>2</sub>-WSe<sub>2</sub> lateral
HSs are grown by pulsed-laser-deposition-assisted selenization method.
The sharp interface of the lateral HS is verified by morphological
and optical characterizations. Intriguingly, photoluminescence spectra
acquired from the interface show rather clear signatures of pristine
MoSe<sub>2</sub> and WSe<sub>2</sub> with no intermediate energy peak
related to intralayer excitonic matter or formation of Mo<sub><i>x</i></sub>W<sub>(1–<i>x</i>)</sub>Se<sub>2</sub> alloys, thereby confirming the sharp interface. Furthermore, the
discrete nature of laterally attached TMDC monolayers, each with doubly
degenerated but nonequivalent energy valleys marked by (<i>K</i><sub>M</sub>, <i>K</i>′<sub>M</sub>) for MoSe<sub>2</sub> and (<i>K</i><sub>W</sub>, <i>K</i>′<sub>W</sub>) for WSe<sub>2</sub> in <i>k</i> space, allows
simultaneous control of the four valleys within the excitation area
without any crosstalk effect over the interface. As an example, <i>K</i><sub>M</sub> and <i>K</i><sub>W</sub> valleys
or <i>K</i>′<sub>M</sub> and <i>K</i>′<sub>W</sub> valleys are simultaneously polarized by controlling the helicity
of circularly polarized optical pumping, where the maximum degree
of polarization is achieved at their respective band edges. The current
work provides the growth mechanism of laterally sharp HSs and highlights
their potential use in valleytronics