4 research outputs found
Improved Growth Behavior of Atomic-Layer-Deposited High‑<i>k</i> Dielectrics on Multilayer MoS<sub>2</sub> by Oxygen Plasma Pretreatment
We
report on the effect of oxygen plasma treatment of two-dimensional
multilayer MoS<sub>2</sub> crystals on the subsequent growth of Al<sub>2</sub>O<sub>3</sub> and HfO<sub>2</sub> films, which were formed
by atomic layer deposition (ALD) using trimethylaluminum and tetrakis-(ethylmethylamino)Âhafnium
metal precursors, respectively, with water oxidant. Due to the formation
of an ultrathin Mo-oxide layer on the MoS<sub>2</sub> surface, the
surface coverage
of Al<sub>2</sub>O<sub>3</sub> and HfO<sub>2</sub> films was significantly
improved compared to those on pristine MoS<sub>2</sub>, even at a
high ALD temperature. These results indicate that the surface modification
of MoS<sub>2</sub> by oxygen plasma treatment can have a major impact
on the subsequent deposition of high-<i>k</i> thin films,
with important implications on their integration in thin film transistors
Chemical Doping Effects in Multilayer MoS<sub>2</sub> and Its Application in Complementary Inverter
Multilayer MoS<sub>2</sub> has been gaining interest as a new semiconducting material
for flexible displays, memory devices, chemical/biosensors, and photodetectors.
However, conventional multilayer MoS<sub>2</sub> devices have exhibited
limited performances due to the Schottky barrier and defects. Here,
we demonstrate polyÂ(diketopyrrolopyrrole-terthiophene) (PDPP3T) doping
effects in multilayer MoS<sub>2</sub>, which results in improved electrical
characteristics (∼4.6× higher on-current compared to the
baseline and a high current on/off ratio of 10<sup>6</sup>). Synchrotron-based
study using X-ray photoelectron spectroscopy and grazing incidence
wide-angle X-ray diffraction provides mechanisms that align the edge-on
crystallites (97.5%) of the PDPP3T as well as a larger interaction
with MoS<sub>2</sub> that leads to dipole and charge transfer effects
(at annealing temperature of 300 °C), which support the observed
enhancement of the electrical characteristics. Furthermore, we demonstrate
a complementary metal–oxide–semiconductor inverter that
uses a p-type MoSe<sub>2</sub> and a PDPP3T-doped MoS<sub>2</sub> as
charging and discharging channels, respectively
Tuning the Built-in Electric Field in Ferroelectric Pb(Zr<sub>0.2</sub>Ti<sub>0.8</sub>)O<sub>3</sub> Films for Long-Term Stability of Single-Digit Nanometer Inverted Domains
The emergence of new technologies, such as whole genome
sequencing
systems, which generate a large amount of data, is requiring ultrahigh
storage capacities. Due to their compactness and low power consumption,
probe-based memory devices using PbÂ(Zr<sub>0.2</sub>Ti<sub>0.8</sub>)ÂO<sub>3</sub> (PZT) ferroelectric films are the ideal candidate
for such applications where portability is desired. To achieve ultrahigh
(>1 Tbit/in<sup>2</sup>) storage densities, sub-10 nm inverted
domains
are required. However, such domains remain unstable and can invert
back to their original polarization due to the effects of an antiparallel
built-in electric field in the PZT film, domain-wall, and depolarization
energies. Here, we show that the built-in electric-field can be tuned
and suppressed by repetitive hydrogen and oxygen plasma treatments.
Such treatments trigger reversible Pb reduction/oxidation activity,
which alters the electrochemistry of the Pb overlayer and compensates
for charges induced by the Pb vacancies. This tuning mechanism is
used to demonstrate the writing of stable and equal size sub-4 nm
domains in both up- and down-polarized PZT films, corresponding to
eight inverted unit-cells. The bit sizes recorded here are the smallest
ever achieved, which correspond to potential 60 Tbit/in<sup>2</sup> data storage densities
Improving the Stability of High-Performance Multilayer MoS<sub>2</sub> Field-Effect Transistors
In
this study, we propose a method for improving the
stability of multilayer MoS<sub>2</sub> field-effect transistors (FETs)
by O<sub>2</sub> plasma treatment and Al<sub>2</sub>O<sub>3</sub> passivation
while sustaining the high performance of bulk MoS<sub>2</sub> FET.
The MoS<sub>2</sub> FETs were exposed to O<sub>2</sub> plasma for
30 s before Al<sub>2</sub>O<sub>3</sub> encapsulation to achieve a
relatively small hysteresis and high electrical performance. A MoO<i><sub>x</sub></i> layer formed during the plasma treatment was
found between MoS<sub>2</sub> and the top passivation layer. The MoO<i><sub>x</sub></i> interlayer prevents the generation of excess
electron carriers in the channel, owing to Al<sub>2</sub>O<sub>3</sub> passivation, thereby minimizing the shift in the threshold voltage
(<i>V</i><sub>th</sub>) and increase of the off-current
leakage. However, prolonged exposure of the MoS<sub>2</sub> surface
to O<sub>2</sub> plasma (90 and 120 s) was found to introduce excess
oxygen into the MoO<i><sub>x</sub></i> interlayer, leading
to more pronounced hysteresis and a high off-current. The stable MoS<sub>2</sub> FETs were also subjected to gate-bias stress tests under
different conditions. The MoS<sub>2</sub> transistors exhibited negligible
decline in performance under positive bias stress, positive bias illumination
stress, and negative bias stress, but large negative shifts in <i>V</i><sub>th</sub> were observed under negative bias illumination
stress, which is attributed to the presence of sulfur vacancies. This
simple approach can be applied to other transition metal dichalcogenide
materials to understand their FET properties and reliability, and
the resulting high-performance hysteresis-free MoS<sub>2</sub> transistors
are expected to open up new opportunities for the development of sophisticated
electronic applications