6 research outputs found
Effects of Excitonic Resonance on Second and Third Order Nonlinear Scattering from Few-Layer MoS<sub>2</sub>
Nonlinear
optical scattering from single- and few-layer MoS<sub>2</sub> contains
important information about the orientation, inversion
symmetry, and degree of interlayer coupling between the layers. We
simultaneously map second harmonic generation (SHG) and four wave
mixing (FWM) signals in chemical vapor deposition (CVD) grown 2H-phase
MoS<sub>2</sub> from single to five layers. We tune the excitation
wavelengths to compare cases where the nonlinear signals are on and
off resonance with the <i>A</i>-exciton band. The SHG signal
shows the expected 4-fold symmetry, however, the FWM signal depends
on the incident laser polarization only, and is independent of the
crystallographic orientation. We show using the symmetry of the Ļ<sup>(3)</sup> tensor that this results from out of plane FWM dipoles.
We explore the scaling of SHG and FWM signals with layer number on
and off excitonic resonance When a nonlinear scattered signal overlaps
with the <i>A</i> excitonic band, the scaling of the signals
with layer number deviates from the expected values, due to the layer
dependent red shift in the exciton absorption peak due to interlayer
coupling. Finally we show that circularly polarized excitation significantly
enhances nonlinear scattering which overlaps with the <i>A</i> excitonic band and indicates the presence of spin splitting of valence
bands at the energy degenerate points (<i>K</i>, <i>K</i>ā²) of the Brillouin zone
Effects of Excitonic Resonance on Second and Third Order Nonlinear Scattering from Few-Layer MoS<sub>2</sub>
Nonlinear
optical scattering from single- and few-layer MoS<sub>2</sub> contains
important information about the orientation, inversion
symmetry, and degree of interlayer coupling between the layers. We
simultaneously map second harmonic generation (SHG) and four wave
mixing (FWM) signals in chemical vapor deposition (CVD) grown 2H-phase
MoS<sub>2</sub> from single to five layers. We tune the excitation
wavelengths to compare cases where the nonlinear signals are on and
off resonance with the <i>A</i>-exciton band. The SHG signal
shows the expected 4-fold symmetry, however, the FWM signal depends
on the incident laser polarization only, and is independent of the
crystallographic orientation. We show using the symmetry of the Ļ<sup>(3)</sup> tensor that this results from out of plane FWM dipoles.
We explore the scaling of SHG and FWM signals with layer number on
and off excitonic resonance When a nonlinear scattered signal overlaps
with the <i>A</i> excitonic band, the scaling of the signals
with layer number deviates from the expected values, due to the layer
dependent red shift in the exciton absorption peak due to interlayer
coupling. Finally we show that circularly polarized excitation significantly
enhances nonlinear scattering which overlaps with the <i>A</i> excitonic band and indicates the presence of spin splitting of valence
bands at the energy degenerate points (<i>K</i>, <i>K</i>ā²) of the Brillouin zone
Effects of Excitonic Resonance on Second and Third Order Nonlinear Scattering from Few-Layer MoS<sub>2</sub>
Nonlinear
optical scattering from single- and few-layer MoS<sub>2</sub> contains
important information about the orientation, inversion
symmetry, and degree of interlayer coupling between the layers. We
simultaneously map second harmonic generation (SHG) and four wave
mixing (FWM) signals in chemical vapor deposition (CVD) grown 2H-phase
MoS<sub>2</sub> from single to five layers. We tune the excitation
wavelengths to compare cases where the nonlinear signals are on and
off resonance with the <i>A</i>-exciton band. The SHG signal
shows the expected 4-fold symmetry, however, the FWM signal depends
on the incident laser polarization only, and is independent of the
crystallographic orientation. We show using the symmetry of the Ļ<sup>(3)</sup> tensor that this results from out of plane FWM dipoles.
We explore the scaling of SHG and FWM signals with layer number on
and off excitonic resonance When a nonlinear scattered signal overlaps
with the <i>A</i> excitonic band, the scaling of the signals
with layer number deviates from the expected values, due to the layer
dependent red shift in the exciton absorption peak due to interlayer
coupling. Finally we show that circularly polarized excitation significantly
enhances nonlinear scattering which overlaps with the <i>A</i> excitonic band and indicates the presence of spin splitting of valence
bands at the energy degenerate points (<i>K</i>, <i>K</i>ā²) of the Brillouin zone
Effects of Excitonic Resonance on Second and Third Order Nonlinear Scattering from Few-Layer MoS<sub>2</sub>
Nonlinear
optical scattering from single- and few-layer MoS<sub>2</sub> contains
important information about the orientation, inversion
symmetry, and degree of interlayer coupling between the layers. We
simultaneously map second harmonic generation (SHG) and four wave
mixing (FWM) signals in chemical vapor deposition (CVD) grown 2H-phase
MoS<sub>2</sub> from single to five layers. We tune the excitation
wavelengths to compare cases where the nonlinear signals are on and
off resonance with the <i>A</i>-exciton band. The SHG signal
shows the expected 4-fold symmetry, however, the FWM signal depends
on the incident laser polarization only, and is independent of the
crystallographic orientation. We show using the symmetry of the Ļ<sup>(3)</sup> tensor that this results from out of plane FWM dipoles.
We explore the scaling of SHG and FWM signals with layer number on
and off excitonic resonance When a nonlinear scattered signal overlaps
with the <i>A</i> excitonic band, the scaling of the signals
with layer number deviates from the expected values, due to the layer
dependent red shift in the exciton absorption peak due to interlayer
coupling. Finally we show that circularly polarized excitation significantly
enhances nonlinear scattering which overlaps with the <i>A</i> excitonic band and indicates the presence of spin splitting of valence
bands at the energy degenerate points (<i>K</i>, <i>K</i>ā²) of the Brillouin zone
High-Performance Hybrid Electronic Devices from Layered PtSe<sub>2</sub> Films Grown at Low Temperature
Layered
two-dimensional (2D) materials display great potential
for a range of applications, particularly in electronics. We report
the large-scale synthesis of thin films of platinum diselenide (PtSe<sub>2</sub>), a thus far scarcely investigated transition metal dichalcogenide.
Importantly, the synthesis by thermally assisted conversion is performed
at 400 Ā°C, representing a breakthrough for the direct integration
of this material with silicon (Si) technology. Besides the thorough
characterization of this 2D material, we demonstrate its promise for
applications in high-performance gas sensing with extremely short
response and recovery times observed due to the 2D nature of the films.
Furthermore, we realized vertically stacked heterostructures of PtSe<sub>2</sub> on Si which act as both photodiodes and photovoltaic cells.
Thus, this study establishes PtSe<sub>2</sub> as a potential candidate
for next-generation sensors and (opto-)Āelectronic devices, using fabrication
protocols compatible with established Si technologies
Direct Observation of Degenerate Two-Photon Absorption and Its Saturation in WS<sub>2</sub> and MoS<sub>2</sub> Monolayer and Few-Layer Films
The optical nonlinearity of WS<sub>2</sub> and MoS<sub>2</sub> monolayer and few-layer films was investigated using the <i>Z</i>-scan technique with femtosecond pulses from the visible to the near-infrared range. The nonlinear absorption of few- and multilayer WS<sub>2</sub> and MoS<sub>2</sub> films and their dependences on excitation wavelength were studied. WS<sub>2</sub> films with 1ā3 layers exhibited a giant two-photon absorption (TPA) coefficient as high as (1.0 Ā± 0.8) Ć 10<sup>4</sup> cm/GW. TPA saturation was observed for the WS<sub>2</sub> film with 1ā3 layers and for the MoS<sub>2</sub> film with 25ā27 layers. The giant nonlinearity of WS<sub>2</sub> and MoS<sub>2</sub> films is attributed to a two-dimensional confinement, a giant exciton effect, and the band edge resonance of TPA