3 research outputs found
Enhancing Surface-Enhanced Raman Scattering Intensity through Light Diffuse Reflection on Ag/ZnO Nanowire Arrays
In this study, we present a new strategy to enhance the
intensity
of surface-enhanced Raman scattering (SERS) signals by using three-dimensional
aggregated silver nanoparticles (AgNPs) on the zinc oxide nanowire
arrays (Ag/ZnO NWA). The ZnO NWA acts as a light-scattering substrate,
providing multidirectional incident light and reflecting a portion
of the Raman scattered light, resulting in an improved SERS signal
intensity. The composite nanowire structure of the Ag/ZnO NWA was
successfully fabricated, and 400 nm ZnO nanowires in the Ag/ZnO NWA
exhibit optimal diffuse light reflection, resulting in a significant
improvement of the SERS signal intensity. The SERS enhancement factor
(EF) for the Ag/ZnO NWA was determined to be EF (ISERS/NSERS)/(IRaman/NRaman) = 3.5 ×
106. This substrate generated a ∼7.9-fold increased
SERS signal compared to the preaggregated AgNPs in the absence of
the ZnO NWA. The detection limit of the Ag/ZnO NWA was estimated by
measuring SERS spectra of rhodamine B, enabling discrimination down
to 10–15 M. Our approach inducing multidirectional
diffuse reflection light to SERS hot spots provides a simple and efficient
strategy to enhance SERS signal intensity, with broad implications
for other spectroscopic applications
Enhancement of Light Absorption in Silicon Nanowire Photovoltaic Devices with Dielectric and Metallic Grating Structures
We report the enhancement
of light absorption in Si nanowire photovoltaic
devices with one-dimensional dielectric or metallic gratings that
are fabricated by a damage-free, precisely aligning, polymer-assisted
transfer method. Incorporation of a Si<sub>3</sub>N<sub>4</sub> grating
with a Si nanowire effectively enhances the photocurrents for transverse-electric
polarized light. The wavelength at which a maximum photocurrent is
generated is readily tuned by adjusting the grating pitch. Moreover,
the electrical properties of the nanowire devices are preserved before
and after transferring the Si<sub>3</sub>N<sub>4</sub> gratings onto
Si nanowires, ensuring that the quality of pristine nanowires is not
degraded during the transfer. Furthermore, we demonstrate Si nanowire
photovoltaic devices with Ag gratings using the same transfer method.
Measurements on the fabricated devices reveal approximately 27.1%
enhancement in light absorption compared to that of the same devices
without the Ag gratings without any degradation of electrical properties.
We believe that our polymer-assisted transfer method is not limited
to the fabrication of grating-incorporated nanowire photovoltaic devices
but can also be generically applied for the implementation of complex
nanoscale structures toward the development of multifunctional optoelectronic
devices
Switching of Photonic Crystal Lasers by Graphene
Unique features of graphene have
motivated the development of graphene-integrated photonic devices.
In particular, the electrical tunability of graphene loss enables
high-speed modulation of light and tuning of cavity resonances in
graphene-integrated waveguides and cavities. However, efficient control
of light emission such as lasing, using graphene, remains a challenge.
In this work, we demonstrate on/off switching of single- and double-cavity
photonic crystal lasers by electrical gating of a monolayer graphene
sheet on top of photonic crystal cavities. The optical loss of graphene
was controlled by varying the gate voltage <i>V</i><sub>g</sub>, with the ion gel atop the graphene sheet. First, the fundamental
properties of graphene were investigated through the transmittance
measurement and numerical simulations. Next, optically pumped lasing
was demonstrated for a graphene-integrated single photonic crystal
cavity at <i>V</i><sub>g</sub> below −0.6 V, exhibiting
a low lasing threshold of ∼480 μW, whereas lasing was
not observed at <i>V</i><sub>g</sub> above −0.6 V
owing to the intrinsic optical loss of graphene. Changing quality
factor of the graphene-integrated photonic crystal cavity enables
or disables the lasing operation. Moreover, in the double-cavity photonic
crystal lasers with graphene, switching of individual cavities with
separate graphene sheets was achieved, and these two lasing actions
were controlled independently despite the close distance of ∼2.2
μm between adjacent cavities. We believe that our simple and
practical approach for switching in graphene-integrated active photonic
devices will pave the way toward designing high-contrast and ultracompact
photonic integrated circuits