8 research outputs found
Supplementary document for Two-dimensional guided-mode resonance gratings with an etch-stop layer and high tolerance to fabrication errors - 5855838.pdf
Supplement
Supplementary document for Grayscale-patterned integrated multilayer-metal-dielectric microcavities for on-chip multi/hyperspectral imaging in the extended visible bandwidth - 6253787.pdf
Supplemental document
Ionic Solvent-Assisted MAPbBr<sub>3</sub> Perovskite Film for Two-Photon Pumped Single-Mode Laser
Miniaturized coherent light sources on the nanoscale
are highly
desired for on-chip photonics integration. However, when approaching
the diffraction limit, the sub-wavelength-scale all-dielectric lasers
are difficult to realize due to the trade-off between lasing performance
and physical size. Especially for a thin-film laser, usually an externally
complex cavity is required to provide the necessary optical feedback.
Herein, we successfully shrink the MAPbBr3 perovskite thin-film
laser to sub-wavelength scale (300 nm) with simplified cavity design
using only an ultraviolet glue layer and a quartz glass. The morphology
quality and the gain properties of the film are enhanced by introducing
ionic liquid. Consequently, the stable and low-threshold single-mode
laser with a highly linear polarization degree of 78.6% and a narrow
line width of 0.35 nm is achieved under two-photon excitation. The
excellent single-mode laser with sub-wavelength scale and ultrasimplified
structure could provide a facile and versatile platform for future
integrated optoelectronic devices
Supplementary document for Design of arbitrary energy distribution beam splitters base on metagratings with multilayer by a hybrid evolutionary particle swarm algorithm - 6685021.pdf
revised versio
Supplementary document for Broadband depolarized perfect Littrow diffraction with multilayer freeform metagratings - 6380604.pdf
Supplementary Figures and Note
Thermally Evaporated MAPbBr<sub>3</sub> Perovskite Random Laser with Improved Speckle-Free Laser Imaging
Metal
halide perovskites (MHPs) are very promising materials for
lasing applications due to their remarkable optical gain properties.
Currently, most perovskite-based lasers are fabricated using lab-scale
solution processing methods. The thermal evaporation (TE) method could
be a promising alternative technology for scale-up fabrication with
significantly improved reproducibility. Unfortunately, the fast and
uncontrollable crystal growth process in thermal evaporation leads
to defective films, and hence their laser performance usually falls
behind their solution-processed counterparts. Here, we demonstrate
high-performance random lasers and explore their speckle-free imaging
application from perovskite thin films fabricated by an improved tri-source
thermal co-evaporation approach assisted by a multifunctional Lewis
base additive, triphenylphosphine oxide (TPPO). The optical gain of
TPPO-passivated MAPbBr3 perovskite films is as high as
∼5 times that of the pristine one, and the corresponding gain
lifetime is almost doubled after TPPO passivation. Due to the small
grain size and compact confinement-induced strong multiple scattering,
a random laser with threshold reduced by half and a high polarization
degree of 78.4% is realized in thermally evaporated MAPbBr3:TPPO perovskite films. These findings would provide a possible route
to scale up the manufacturing of high-performance perovskite materials
and devices and open new perspectives for integrated speckle-free
laser imaging systems
Random Lasing from Thermally Evaporated Quasi-Two-Dimensional Perovskite Film for Speckle-free Imaging
Quasi-two-dimensional (quasi-2D) perovskites are promising
as a
gain medium for laser applications owing to their inherent multiple
quantum wells and remarkable stability. Meanwhile, thermal evaporation
deposition is a promising complementary approach to further advance
the commercialization of perovskite-based lasers. However, investigations
into thermally evaporated perovskite lasers are scarce, and their
performance is significantly inferior to that of their solution-processed
counterparts. Herein, we demonstrate a high-quality thermally evaporated
quasi-2D perovskite film with excellent gain properties via a tri-source
co-evaporation strategy. The carrier dynamics and gain nature of the
perovskite film are revealed with a long gain lifetime of 66.5 ps.
The net modal gain is up to 1071 cm–1, which is
afforded by rapid carrier accumulation (<0.25 ps) and facile buildup
of population inversion. As a result, random lasing from the quasi-2D
perovskite film with a low threshold of 10.39 μJ/cm2 is achieved. Furthermore, under the illumination of random lasing,
clear speckle-free imaging with an impressively low speckle contrast
of C ∼ 0 is demonstrated. This work highlights
the possibility of using thermally evaporated perovskites for the
development of high-performance random lasers and integrated speckle-free
imaging systems
Gate-Tuning Hybrid Polaritons in Twisted α‑MoO<sub>3</sub>/Graphene Heterostructures
Modulating
anisotropic phonon polaritons (PhPs) can open new avenues
in infrared nanophotonics. Promising PhP dispersion engineering through
polariton hybridization has been demonstrated by coupling gated graphene
to single-layer α-MoO3. However, the mechanism underlying
the gate-dependent modulation of hybridization has remained elusive.
Here, using IR nanospectroscopic imaging, we demonstrate active modulation
of the optical response function, quantified in measurements of gate
dependence of wavelength, amplitude, and dissipation rate of the hybrid
plasmon–phonon polaritons (HPPPs) in both single-layer and
twisted bilayer α-MoO3/graphene heterostructures.
Intriguingly, while graphene doping leads to a monotonic increase
in HPPP wavelength, amplitude and dissipation rate show transition
from an initially anticorrelated decrease to a correlated increase.
We attribute this behavior to the intricate interplay of gate-dependent
components of the HPPP complex momentum. Our results provide the foundation
for active polariton control of integrated α-MoO3 nanophotonics devices
