182 research outputs found
Electric Field Induced Schottky to Ohmic Contact Transition in Fe<sub>3</sub>GeTe<sub>2</sub>/TMDs Contacts
Although the two-dimensional transition
metal dichalcogenides
(TMDs)
present excellent electrical properties, the contact resistance at
the interface of metal/TMDs limits the device performance. Herein,
we use 2D metallic Fe3GeTe2 (FGT) as an electrode
in contact with TMDs semiconductors MX2 (M = Mo, W; X =
S, Se, Te) and investigate the contact properties of FGT/MX2 based on density functional theory calculations. We demonstrated
that FGT/MX2 presents n-type Schottky contacts, and their
n-type Schottky barrier heights are lower than that of the most common
bulk metal contacts with MX2, suggesting that FGT can be
used as an efficient metallic electrode for MX2. The transitions
from n-type Schottky contact to p-type Schottky contact and from Schottky
contact to Ohmic contact can be achieved in FGT/MX2 under
the electric field. This work not only illustrates an effective method
to modulate the contact types and Schottky barrier heights of FGT/MX2 contacts but also provides a route for designing the nanodevices
based on FGT/MX2 electrical contacts
New Insights into Electrochemical Lithiation/Delithiation Mechanism of α‑MoO<sub>3</sub> Nanobelt by in Situ Transmission Electron Microscopy
The α-MoO3 nanobelt
has great potential for application as anode of lithium ion batteries
(LIBs) because of its high capacity and unique one-dimensional layer
structure. However, its fundmental electrochemical failure mechanism
during first lithiation/delithiation process is still unclear. Here,
we constructed an electrochemical setup within α-MoO3 nanobelt anode inside a transmission electron microscope to observe
in situ the mircostructure evolution during cycles. Upon first lithiation,
the α-MoO3 nanobelt converted into numerous Mo nanograins
within the Li2O matrix, with an obvious size expansion.
Interestingly, α-MoO3 nanobelt was found to undergo
a two-stage delithiation process. Mo nanograins were first transformed
into crystalline Li1.66Mo0.66O2 along
with the disappearance of Li2O and size shrink, followed
by the conversion to amorphous Li2MoO3. This
irreversible phase conversion should be responsible for the large
capacity loss in first cycle. In addition, a fully reversile phase
conversion between crystalline Mo and amorphous Li2MoO3 was revealed accompanying the formation and disapperance
of the Li2O layer during the subsequent cycles. Our experiments
provide direct evidence to deeply understand the distinctive electrochemical
lithiation/delithiation behaviors of α-MoO3 nanobelt,
shedding light onto the development of α-MoO3 anode
for LIBs
Fluorine-Ion-Mediated Electrodeposition of Rhombus-Like ZnFOH Nanorod Arrays: An Intermediate Route to Novel ZnO Nanoarchitectures
Novel rhombus-like ZnO nanorod (NR) arrays were achieved via a facile two-step synthesis strategy based on first a low-temperature aqueous electrodeposition of vertically aligned rhombic ZnFOH NR arrays in the presence of fluoride and second a pyrolysis of ZnFOH intermediate into ZnO with the same morphology. The fluorine-ion-mediated electrodeposition mechanism of ZnFOH was confirmed for the first time, and the proposed formation process that the rhombus-like ZnO NRs characterized by mesoporous structure derived from the electrodeposited ZnFOH intermediate was corroborated by systematic structural characterization of the as-prepared products. A dye-sensitized solar cell (DSSC) based on the rhombus-like ZnO NR arrays with a larger surface roughness factor was assembled, and a higher conversion efficiency of 0.69% was attained in comparison to 0.47% of the DSSC based on the hexagon-like ZnO NR arrays electrodeposited in the absence of fluoride. Further, we demonstrate that the unique two-step synthesis strategy also possessed the capability of constructing complex nanoarchitectures with 1D rhombus-like ZnO NRs as the building blocks
New Insights into Electrochemical Lithiation/Delithiation Mechanism of α‑MoO<sub>3</sub> Nanobelt by in Situ Transmission Electron Microscopy
The α-MoO3 nanobelt
has great potential for application as anode of lithium ion batteries
(LIBs) because of its high capacity and unique one-dimensional layer
structure. However, its fundmental electrochemical failure mechanism
during first lithiation/delithiation process is still unclear. Here,
we constructed an electrochemical setup within α-MoO3 nanobelt anode inside a transmission electron microscope to observe
in situ the mircostructure evolution during cycles. Upon first lithiation,
the α-MoO3 nanobelt converted into numerous Mo nanograins
within the Li2O matrix, with an obvious size expansion.
Interestingly, α-MoO3 nanobelt was found to undergo
a two-stage delithiation process. Mo nanograins were first transformed
into crystalline Li1.66Mo0.66O2 along
with the disappearance of Li2O and size shrink, followed
by the conversion to amorphous Li2MoO3. This
irreversible phase conversion should be responsible for the large
capacity loss in first cycle. In addition, a fully reversile phase
conversion between crystalline Mo and amorphous Li2MoO3 was revealed accompanying the formation and disapperance
of the Li2O layer during the subsequent cycles. Our experiments
provide direct evidence to deeply understand the distinctive electrochemical
lithiation/delithiation behaviors of α-MoO3 nanobelt,
shedding light onto the development of α-MoO3 anode
for LIBs
Ultralow Contact Resistance and Efficient Ohmic Contacts in MoGe<sub>2</sub>P<sub>4</sub>–Metal Contacts
The
MoGe2P4 monolayer, an emerging semiconductor
with high carrier mobility, can be proposed as a promising channel
material in field effect transistors (FETs). The contact resistance
between MoGe2P4 and the metal electrode will
limit the performance of a realistic FET. Using density functional
theory (DFT) calculations, we explore the contact properties of a
MoGe2P4 monolayer with six bulk metal electrodes
(In, Ag, Au, Cu, Pd, and Pt). It is demonstrated that the Ohmic contacts
are formed in all MoGe2P4–metal contacts
due to the strong interfacial interactions, suggesting the high carrier
injection efficiency. In addition, the MoGe2P4–Cu, −Pd, and −Pt contacts present 100% tunneling
probability due to the absence of the tunneling barrier width. The
tunneling probabilities of the MGP–In, MGP–Ag, and MGP–Au
contacts are exceptionally higher than those of most other 2D semiconductors.
Moreover, the tunneling-specific resistivity of all MoGe2P4–metal contacts is relatively low, indicating
an ultralow contact resistance and excellent performance. These findings
provide a useful guideline to design high-performance MoGe2P4-based electronic devices
Semiconductor to Metal to Half-Metal Transition in Pt-Embedded Zigzag Graphene Nanoribbons
The electronic and magnetic properties
of Pt-embedded zigzag graphene nanoribbons (Pt–ZGNRs) are investigated
using density-functional theory calculations. It is found that Pt–ZGNRs
exhibit a semiconductor–metal–half-metal transition
as the position of Pt substitutional impurities in the ribbon changes
from the center to edge sites. This behavior can be attributed to
the interaction between Pt impurities and edge states of ZGNRs, which
governs the electron occupation of the edge states. The transition
always occurs independent of ribbon width. However, Pt impurity concentration
is important for obtaining this transition. Our results demonstrate
that Pt–ZGNRs can be used as versatile electronic devices
Tunable Schottky Barrier and Efficient Ohmic Contacts in MSi<sub>2</sub>N<sub>4</sub> (M = Mo, W)/2D Metal Contacts
Monolayer MSi2N4 (M = Mo, W) has
been fabricated
and proposed as a promising channel material for field-effect transistors
(FETs) due to the high electron/hole mobility. However, the barrier
between the metal electrode and MSi2N4 will
affect device performance. Hence, it is desirable to reduce the barrier
for achieving high-performance electrical devices. Here, using density
functional theory (DFT) calculations, we systematically investigate
the electrical properties of the van der Waals (vdW) contacts formed
between MSi2N4 and two-dimensional (2D) metals
(XY2, X = Nb, Ta, Y = S, Se, Te). It is found that the
contact types and Schottky barrier height (SBH) of MSi2N4/XY2 can be effectively tuned by selecting
2D metals with different work functions (WFs). Specifically, n- and
p-type Schottky contacts and Ohmic contacts can be achieved in MSi2N4/XY2. Among them, MoSi2N4/H-NbS2, WSi2N4/H-XS2, and WSi2N4/H-NbSe2 present
Ohmic contacts due to the high WF of 2D metals. Notably, the pinning
factors of MSi2N4/XY2 are obviously
larger than those of the other 2D semiconductor/metal contacts, indicating
that the Fermi-level pinning (FLP) effect is weak in MSi2N4/XY2. Therefore, vdW stack engineering can
strongly weaken the FLP effect, making the Schottky barrier tunable
in MSi2N4/XY2 by choosing 2D metals
with different WFs. The results provide important insights into the
selection of appropriate electrodes and valuable guidance for the
development of MSi2N4-based 2D electronic devices
with high performance
New Insights into Electrochemical Lithiation/Delithiation Mechanism of α‑MoO<sub>3</sub> Nanobelt by in Situ Transmission Electron Microscopy
The α-MoO<sub>3</sub> nanobelt
has great potential for application as anode of lithium ion batteries
(LIBs) because of its high capacity and unique one-dimensional layer
structure. However, its fundmental electrochemical failure mechanism
during first lithiation/delithiation process is still unclear. Here,
we constructed an electrochemical setup within α-MoO<sub>3</sub> nanobelt anode inside a transmission electron microscope to observe
in situ the mircostructure evolution during cycles. Upon first lithiation,
the α-MoO<sub>3</sub> nanobelt converted into numerous Mo nanograins
within the Li<sub>2</sub>O matrix, with an obvious size expansion.
Interestingly, α-MoO<sub>3</sub> nanobelt was found to undergo
a two-stage delithiation process. Mo nanograins were first transformed
into crystalline Li<sub>1.66</sub>Mo<sub>0.66</sub>O<sub>2</sub> along
with the disappearance of Li<sub>2</sub>O and size shrink, followed
by the conversion to amorphous Li<sub>2</sub>MoO<sub>3</sub>. This
irreversible phase conversion should be responsible for the large
capacity loss in first cycle. In addition, a fully reversile phase
conversion between crystalline Mo and amorphous Li<sub>2</sub>MoO<sub>3</sub> was revealed accompanying the formation and disapperance
of the Li<sub>2</sub>O layer during the subsequent cycles. Our experiments
provide direct evidence to deeply understand the distinctive electrochemical
lithiation/delithiation behaviors of α-MoO<sub>3</sub> nanobelt,
shedding light onto the development of α-MoO<sub>3</sub> anode
for LIBs
Enhanced Thermal Stability of Gold and Silver Nanorods by Thin Surface Layers
Using in situ transmission electron microscopy, we find that a carbon shell governs the morphological transitions
of gold and silver nanorods upon heating. Encapsulated Ag nanorods show a surprising nonuniform sublimation
behavior starting from one side and leaving behind the shell. Uncovered gold nanorods transform their shape
to spheres well below the bulk melting temperature through surface diffusion, which is prevented by a thin
carbon shell
Synthesis of Dumbbell-Shaped Manganese Oxide Nanocrystals
Dumbbell-like homogeneous MnO nanocrystals are obtained for the first time via the pyrolysis of manganese
formate in trioctylamine/oleic acid media and the orientation aggregation mechanism is proposed for this 1D
growth route
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