11 research outputs found
Abrupt metal-insulator transition observed in VO2 thin films induced by a switching voltage pulse
An abrupt metal-insulator transition (MIT) was observed in VO2 thin films
during the application of a switching voltage pulse to two-terminal devices.
Any switching pulse over a threshold voltage for the MIT of 7.1 V enabled the
device material to transform efficiently from an insulator to a metal. The
characteristics of the transformation were analyzed by considering both the
delay time and rise time of the measured current response. The extrapolated
switching time of the MIT decreased down to 9 ns as the external load
resistance decreased to zero. Observation of the intrinsic switching time of
the MIT in the correlated oxide films is impossible because of the
inhomogeneity of the material; both the metallic state and an insulating state
co-exist in the measurement volume. This indicates that the intrinsic switching
time is in the order of less than a nanosecond. The high switching speed might
arise from a strong correlation effect (Coulomb repulsion) between the
electrons in the material.Comment: 5 pages, 5 figure
Observation of First-Order Metal-Insulator Transition without Structural Phase Transition in VO_2
An abrupt first-order metal-insulator transition (MIT) without structural
phase transition is first observed by current-voltage measurements and
micro-Raman scattering experiments, when a DC electric field is applied to a
Mott insulator VO_2 based two-terminal device. An abrupt current jump is
measured at a critical electric field. The Raman-shift frequency and the
bandwidth of the most predominant Raman-active A_g mode, excited by the
electric field, do not change through the abrupt MIT, while, they, excited by
temperature, pronouncedly soften and damp (structural MIT), respectively. This
structural MIT is found to occur secondarily.Comment: 4 pages, 4 figure
Observation of Mott Transition in VO_2 Based Transistors
An abrupt Mott metal-insulator transition (MIT) rather than the continuous
Hubbard MIT near a critical on-site Coulomb energy U/U_c=1 is observed for the
first time in VO_2, a strongly correlated material, by inducing holes of about
0.018% into the conduction band. As a result, a discontinuous jump of the
density of states on the Fermi surface is observed and inhomogeneity inevitably
occurs. The gate effect in fabricated transistors is clear evidence that the
abrupt MIT is induced by the excitation of holes.Comment: 4 pages, 4 figure
Junctionless Diode Enabled by Self-Bias Effect of Ion Gel in Single-Layer MoS<sub>2</sub> Device
The self-biasing
effects of ion gel from source and drain electrodes on electrical
characteristics of single layer and few layer molybdenum disulfide
(MoS<sub>2</sub>) field-effect transistor (FET) have been studied.
The self-biasing effect of ion gel is tested for two different configurations,
covered and open, where ion gel is in contact with either one or both,
source and drain electrodes, respectively. In open configuration,
the linear output characteristics of the pristine device becomes nonlinear
and on–off ratio drops by 3 orders of magnitude due to the
increase in “off” current for both single and few layer
MoS<sub>2</sub> FETs. However, the covered configuration results in
a highly asymmetric output characteristics with a rectification of
around 10<sup>3</sup> and an ideality factor of 1.9. This diode like
behavior has been attributed to the reduction of Schottky barrier
width by the electric field of self-biased ion gel, which enables
an efficient injection of electrons by tunneling at metal-MoS<sub>2</sub> interface. Finally, finite element method based simulations
are carried out and the simulated results matches well in principle
with the experimental analysis. These self-biased diodes can perform
a crucial role in the development of high-frequency optoelectronic
and valleytronic devices
Tunable Electron and Hole Injection Enabled by Atomically Thin Tunneling Layer for Improved Contact Resistance and Dual Channel Transport in MoS<sub>2</sub>/WSe<sub>2</sub> van der Waals Heterostructure
Two-dimensional
(2D) material-based heterostructures provide a unique platform where
interactions between stacked 2D layers can enhance the electrical
and opto-electrical properties as well as give rise to interesting
new phenomena. Here, the operation of a van der Waals heterostructure
device comprising of vertically stacked bilayer MoS<sub>2</sub> and
few layered WSe<sub>2</sub> has been demonstrated in which an atomically
thin MoS<sub>2</sub> layer has been employed as a tunneling layer
to the underlying WSe<sub>2</sub> layer. In this way, simultaneous
contacts to both MoS<sub>2</sub> and WSe<sub>2</sub> 2D layers have
been established by forming a direct metal–semiconductor to
MoS<sub>2</sub> and a tunneling-based metal–insulator–semiconductor
contacts to WSe<sub>2</sub>, respectively. The use of MoS<sub>2</sub> as a dielectric tunneling layer results in an improved contact resistance
(80 kΩ μm) for WSe<sub>2</sub> contact, which is attributed
to reduction in the effective Schottky barrier height and is also
confirmed from the temperature-dependent measurement. Furthermore,
this unique contact engineering and type-II band alignment between
MoS<sub>2</sub> and WSe<sub>2</sub> enables a selective and independent
carrier transport across the respective layers. This contact engineered
dual channel heterostructure exhibits an excellent gate control and
both channel current and carrier types can be modulated by the vertical
electric field of the gate electrode, which is also reflected in the
on/off ratio of 10<sup>4</sup> for both electron (MoS<sub>2</sub>)
and hole (WSe<sub>2</sub>) channels. Moreover, the charge transfer
at the heterointerface is studied quantitatively from the shift in
the threshold voltage of the pristine MoS<sub>2</sub> and the heterostructure
device, which agrees with the carrier recombination-induced optical
quenching as observed in the Raman spectra of the pristine and heterostructure
layers. This observation of dual channel ambipolar transport enabled
by the hybrid tunneling contacts and strong interlayer coupling can
be utilized for high-performance opto-electrical devices and applications
Gate Tunable Self-Biased Diode Based on Few Layered MoS<sub>2</sub> and WSe<sub>2</sub>
The
operation of a self-biased diode (SBD) based on MoS<sub>2</sub> has
been demonstrated by using an asymmetric top gate comprising
metal-hexagonal boron nitride (h-BN)-MoS<sub>2</sub> structure. The
rectification is achieved by asymmetric modulation of effective Schottky
barrier and carrier density in the channel during forward and reverse
bias, and a rectification factor of 1.3 Ă— 10<sup>5</sup> is achieved
in <i>I–V</i> characteristics. The modulation of
effective Schottky barrier is verified by temperature dependent measurement
in a range of 173 to 373 K, and a difference of 300 meV is observed
in effective Schottky barrier height for forward and reverse bias.
The electrical characteristics of SBD exhibit close resemblance with
an ideal thermionic emission model with an ideality factor of 1.3.
SBD also exhibits strong photoelectrical response with a specific
detectivity of 150 A/W and responsivity of 2.1 Ă— 10<sup>10</sup> Jones under 450 nm laser light illumination. In the end, to demonstrate
the diversity of the proposed scheme, SBD based on WSe<sub>2</sub> has also been fabricated and the results have been discussed. These
results suggest a new route toward the SBD based numerous electronics
and optoelectronics applications and can in principle be implemented
using other two-dimensional materials as well