7 research outputs found
Bandgap Extraction and Device Analysis of Ionic Liquid Gated WSe<sub>2</sub> Schottky Barrier Transistors
Through the careful study of ionic
liquid gated WSe<sub>2</sub> Schottky barrier field-effect transistors
as a function of flake
thicknessî—¸referred to in the following as body thickness, <i>t</i><sub>body</sub>î—¸critical insights into the electrical
properties of WSe<sub>2</sub> are gained. One finding is that the
inverse subthreshold slope shows a clear dependence on body thickness, <i>i</i>.<i>e</i>., an approximate square root dependent
increase with <i>t</i><sub>body</sub>, that provides evidence
that injection into the WSe<sub>2</sub> channel is mediated by thermally
assisted tunneling through the gate-controlled Schottky barriers at
the source and drain. By employing our Schottky barrier model, a detailed
experimental plot of the WSe<sub>2</sub> bandgap as a function of
body thickness is obtained. We will discuss why the analysis employed
here is critically dependent on the use of the above-mentioned ionic
liquid gate and how device characteristics are analyzed in detail
High Performance Multilayer MoS<sub>2</sub> Transistors with Scandium Contacts
While there has been growing interest in two-dimensional
(2-D)
crystals other than graphene, evaluating their potential usefulness
for electronic applications is still in its infancy due to the lack
of a complete picture of their performance potential. The focus of
this article is on contacts. We demonstrate that through a proper
understanding and design of source/drain contacts and the right choice
of number of MoS<sub>2</sub> layers the excellent intrinsic properties
of this 2-D material can be harvested. Using scandium contacts on
10-nm-thick exfoliated MoS<sub>2</sub> flakes that are covered by
a 15 nm Al<sub>2</sub>O<sub>3</sub> film, high effective mobilities
of 700 cm<sup>2</sup>/(V s) are achieved at room temperature. This
breakthrough is largely attributed to the fact that we succeeded in
eliminating contact resistance effects that limited the device performance
in the past unrecognized. In fact, the apparent linear dependence
of current on drain voltage had mislead researchers to believe that
a truly Ohmic contact had already been achieved, a misconception that
we also elucidate in the present article
Utilizing Electrical Characteristics of Individual Nanotube Devices to Study the Charge Transfer between CdSe Quantum Dots and Double-Walled Nanotubes
To study the charge transfer between
cadmium selenide (CdSe) quantum
dots (QDs) and double-walled nanotubes (DWNTs), various sizes of CdSe–ligand–DWNT
structures are synthesized, and field-effect transistors from individual
functionalized DWNTs rather than networks of the same are fabricated.
From the electrical measurements, two distinct electron transfer mechanisms
from the QD system to the nanotube are identified. By the formation
of the CdSe–ligand–DWNT heterostructure, an effectively
n-doped nanotube is created due to the smaller work function of CdSe
as compared with that of the nanotube. In addition, once the QD–DWNT
system is exposed to laser light, further electron transfer from the
QD through the ligand, specifically, 4-mercaptophenol (MTH), to the
nanotube occurs and a clear QD size-dependent tunneling process is
observed. The detailed analysis of a large set of devices and the
particular methodology employed here for the first time allowed for
extracting a wavelength and quantum dot size-dependent charge transfer
efficiencyî—¸a quantity that is evaluated for the first time
through electrical measurement
Spin Transfer Torque in a Graphene Lateral Spin Valve Assisted by an External Magnetic Field
Spin-based devices are widely discussed
for post-complementary
metal–oxide–semiconductor (CMOS) applications. A number
of spin device ideas propose using spin current to carry information
coherently through a spin channel and transfering it to an output
magnet by spin transfer torque. Graphene is an ideal channel material
in this context due to its long spin diffusion length, gate-tunable
carrier density, and high carrier mobility. However, spin transfer
torque has not been demonstrated in graphene or any other semiconductor
material as of yet. Here, we report the first experimental measurement
of spin transfer torque in graphene lateral nonlocal spin valve devices.
Assisted by an external magnetic field, the magnetization reversal
of the ferromagnetic receiving magnet is induced by pure spin diffusion
currents from the input magnet. The magnetization switching is reversible
between parallel and antiparallel configurations, depending on the
polarity of the applied charged current. The presented results are
an important step toward developing graphene-based spin logic and
understanding spin-transfer torque in systems with tunneling barriers
Characterization of Single Defects in Ultrascaled MoS<sub><b>2</b></sub> Field-Effect Transistors
MoS<sub>2</sub> has received a lot of attention lately as a semiconducting
channel material for electronic devices, in part due to its large
band gap as compared to that of other 2D materials. Yet, the performance
and reliability of these devices are still severely limited by defects
which act as traps for charge carriers, causing severely reduced mobilities,
hysteresis, and long-term drift. Despite their importance, these defects
are only poorly understood. One fundamental problem in defect characterization
is that due to the large defect concentration only the average response
to bias changes can be measured. On the basis of such averaged data,
a detailed analysis of their properties and identification of particular
defect types are difficult. To overcome this limitation, we here characterize
single defects on MoS<sub>2</sub> devices by performing measurements
on ultrascaled transistors (∼65 × 50 nm) which contain
only a few defects. These single defects are characterized electrically
at varying gate biases and temperatures. The measured currents contain
random telegraph noise, which is due to the transfer of charge between
the channel of the transistors and individual defects, visible only
due to the large impact of a single elementary charge on the local
electrostatics in these small devices. Using hidden Markov models
for statistical analysis, we extract the charge capture and emission
times of a number of defects. By comparing the bias-dependence of
the measured capture and emission times to the prediction of theoretical
models, we provide simple rules to distinguish oxide traps from adsorbates
on these back-gated devices. In addition, we give simple expressions
to estimate the vertical and energetic positions of the defects. Using
the methods presented in this work, it is possible to locate the sources
of performance and reliability limitations in 2D devices and to probe
defect distributions in oxide materials with 2D channel materials
Probing the Dependence of Electron Transfer on Size and Coverage in Carbon Nanotube–Quantum Dot Heterostructures
As a model system for understanding
charge transfer in novel architectural designs for solar cells, double-walled
carbon nanotube (DWNT)–CdSe quantum dot (QD) (QDs with average
diameters of 2.3, 3.0, and 4.1 nm) heterostructures have been fabricated.
The individual nanoscale building blocks were successfully attached
and combined using a hole-trapping thiol linker molecule, i.e., 4-mercaptophenol
(MTH), through a facile, noncovalent π–π stacking
attachment strategy. Transmission electron microscopy confirmed the
attachment of QDs onto the external surfaces of the DWNTs. We herein
demonstrate a meaningful and unique combination of near-edge X-ray
absorption fine structure (NEXAFS) and Raman spectroscopies bolstered
by complementary electrical transport measurements in order to elucidate
the synergistic interactions between CdSe QDs and DWNTs, which are
facilitated by the bridging MTH molecules that can scavenge photoinduced
holes and potentially mediate electron redistribution between the
conduction bands in CdSe QDs and the C 2p-derived states of the DWNTs.
Specifically, we correlated evidence of charge transfer as manifested
by (i) changes in the NEXAFS intensities of π* resonance in
the C <i>K</i>-edge and Cd <i>M</i><sub>3</sub>-edge spectra, (ii) a perceptible outer tube G-band downshift in
frequency in Raman spectra, as well as (iii) alterations in the threshold
characteristics present in transport data as a function of CdSe QD
deposition onto the DWNT surface. In particular, the separate effects
of (i) varying QD sizes and (ii) QD coverage densities on the electron
transfer were independently studied
Covalent Nitrogen Doping and Compressive Strain in MoS<sub>2</sub> by Remote N<sub>2</sub> Plasma Exposure
Controllable doping of two-dimensional
materials is highly desired for ideal device performance in both hetero-
and p-n homojunctions. Herein, we propose an effective strategy for
doping of MoS<sub>2</sub> with nitrogen through a remote N<sub>2</sub> plasma surface treatment. By monitoring the surface chemistry of
MoS<sub>2</sub> upon N<sub>2</sub> plasma exposure using in situ X-ray
photoelectron spectroscopy, we identified the presence of covalently
bonded nitrogen in MoS<sub>2</sub>, where substitution of the chalcogen
sulfur by nitrogen is determined as the doping mechanism. Furthermore,
the electrical characterization demonstrates that p-type doping of
MoS<sub>2</sub> is achieved by nitrogen doping, which is in agreement
with theoretical predictions. Notably, we found that the presence
of nitrogen can induce compressive strain in the MoS<sub>2</sub> structure,
which represents the first evidence of strain induced by substitutional
doping in a transition metal dichalcogenide material. Finally, our
first principle calculations support the experimental demonstration
of such strain, and a correlation between nitrogen doping concentration
and compressive strain in MoS<sub>2</sub> is elucidated