5 research outputs found
Local and Nonlocal Optically Induced Transparency Effects in Graphene–Silicon Hybrid Nanophotonic Integrated Circuits
Graphene is well-known as a two-dimensional sheet of carbon atoms arrayed in a honeycomb structure. It has some unique and fascinating properties, which are useful for realizing many optoelectronic devices and applications, including transistors, photodetectors, solar cells, and modulators. To enhance light–graphene interactions and take advantage of its properties, a promising approach is to combine a graphene sheet with optical waveguides, such as silicon nanophotonic wires considered in this paper. Here we report <i>local</i> and <i>nonlocal</i> optically induced transparency (OIT) effects in graphene–silicon hybrid nanophotonic integrated circuits. A low-power, continuous-wave laser is used as the pump light, and the power required for producing the OIT effect is as low as ∼0.1 mW. The corresponding power density is several orders lower than that needed for the previously reported saturated absorption effect in graphene, which implies a mechanism involving light absorption by the silicon and photocarrier transport through the silicon–graphene junction. The present OIT effect enables low power, all-optical, broadband control and sensing, modulation and switching <i>locally</i> and <i>nonlocally</i>
High-Bandwidth Zero-Biased Waveguide-Integrated p‑n Homojunction Graphene Photodetectors on Silicon for a Wavelength Band of 1.55 μm and Beyond
The
p-n homojunction graphene photodetectors (GPDs) based on the
photothermoelectric (PTE) effect have drawn much attention for featuring
zero-bias operation (i.e., zero dark current) with a bandwidth of
tens of GHz. However, most waveguide-integrated GPDs were demonstrated
for the 1.55 μm wavelength band. Here, we realize high-performance
silicon waveguide integrated GPDs enabling efficient light absorption
at both wavelength bands of 1.55 and 2 μm. The broadband operation
of the present PTE GPDs is analyzed theoretically and experimentally.
When operating at 1.55 μm, the GPD typically exhibits a responsivity
of ∼2.81 V/W and a 3 dB bandwidth of >40 GHz (setup-limited)
under zero bias. When the GPDs operate at 2 μm under zero bias,
the responsivity is about 2.78–4 V/W and the 3 dB bandwidth
is >22 GHz (setup-limited). The measured linear dynamic range is
over
24 dB for both wavelength bands of 1.55 and 2 μm. The present
high-performance waveguide-integrated GPD provides a promising option
for the applications of silicon photonics beyond 1.55 μm, such
as optical communications, photonics sending, etc
Changes in iTRAQ-Based Proteomic Profiling of the Cladoceran <i>Daphnia magna</i> Exposed to Microcystin-Producing and Microcystin-Free <i>Microcystis aeruginosa</i>
Global warming and
increased nutrient
fluxes cause cyanobacterial blooms in freshwater ecosystems. These
phenomena have increased the concern for human health and ecosystem
services. The mass occurrences of toxic cyanobacteria strongly affect
freshwater zooplankton communities, especially the unselective filter
feeder <i>Daphnia</i>. However, the molecular mechanisms
of cyanobacterial toxicity remain poorly understood. This study is
the first to combine the established body growth rate (BGR), which
is an indicator of life-history fitness, with differential peptide
labeling (iTRAQ)-based proteomics in <i>Daphnia magna</i> influenced by microcystin-producing (MP) and microcystin-free (MF) <i>Microcystis aeruginosa</i>. A significant decrease in BGR was
detected when <i>D. magna</i> was exposed to MP or MF <i>M. aeruginosa</i>. Conducting iTRAQ proteomic analyses, we successfully
identified and quantified 211 proteins with significant changes in
expression. A cluster of orthologous groups revealed that <i>M. aeruginosa</i>-affected differential proteins were strongly
associated with lipid, carbohydrate, amino acid, and energy metabolism.
These parameters could potentially explain the reduced fitness based
on the cost of the substance metabolism
Supplement 1: All-optical graphene modulator based on optical Kerr phase shift
Supplemental document for all-optical graphene modulator based
on optical Kerr phase shift. Originally published in Optica on 20 May 2016 (optica-3-5-541