7 research outputs found
Fast Switching “On/Off” Chiral Surface Plasmon Polaritons in Graphene-Coated Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> Nanowire
Plasmonic
nanowire was found to generate chiral surface plasmon
polaritons (SPPs), with the perspective of enhancing molecular spectroscopy
for biosensing applications. However, the lack of chiroptical switches
exhibits significant limitations in detecting a multitude of various
analytes with a high sensitivity and in asymmetric catalysis to provide
a switchable stereoselectivity. Here, we numerically and analytically
propose a graphene-coated Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> (GST225) nanowire to solve this problem. We highlight that the chiral
SPPs propagating along the nanowire can be reversibly switched between
“on” (transparent) and “off” (opaque)
as transiting the state of GST225 core between amorphous and crystalline.
Moreover by changing the Fermi energy of the graphene coating layer,
the hybrid nanowire can produce either achiral or chiral SPPs at the
output of nanowire. A thermal-electric model is put forward to study
the temporal variation of the temperature of the GST225 core. Transiting
the structural phase of GST225 in nanosecond was theoretically demonstrated.
Our proof of concept permits the preparation of circularly polarized
light source with a fast switching “on/off” function.
We foresee its potential applications for tunable nanophotonic devices,
plasmonic nanowire networks, on-chip biosensing, etc., where the active
controlling of SPPs is necessary
Fast Switching “On/Off” Chiral Surface Plasmon Polaritons in Graphene-Coated Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> Nanowire
Plasmonic
nanowire was found to generate chiral surface plasmon
polaritons (SPPs), with the perspective of enhancing molecular spectroscopy
for biosensing applications. However, the lack of chiroptical switches
exhibits significant limitations in detecting a multitude of various
analytes with a high sensitivity and in asymmetric catalysis to provide
a switchable stereoselectivity. Here, we numerically and analytically
propose a graphene-coated Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> (GST225) nanowire to solve this problem. We highlight that the chiral
SPPs propagating along the nanowire can be reversibly switched between
“on” (transparent) and “off” (opaque)
as transiting the state of GST225 core between amorphous and crystalline.
Moreover by changing the Fermi energy of the graphene coating layer,
the hybrid nanowire can produce either achiral or chiral SPPs at the
output of nanowire. A thermal-electric model is put forward to study
the temporal variation of the temperature of the GST225 core. Transiting
the structural phase of GST225 in nanosecond was theoretically demonstrated.
Our proof of concept permits the preparation of circularly polarized
light source with a fast switching “on/off” function.
We foresee its potential applications for tunable nanophotonic devices,
plasmonic nanowire networks, on-chip biosensing, etc., where the active
controlling of SPPs is necessary
Wideband Absorbers in the Visible with Ultrathin Plasmonic-Phase Change Material Nanogratings
The narrowband surface plasmon resonance
of metallic nanostructures
was once thought to limit the bandwidth of absorptance, yet recent
demonstrations show that it can be harnessed using mechanisms such
as multiple resonances, impedance matching, and slow-light modes to
create broadband absorptance. However, in the visible spectrum, realization
of absorbers based on patterned plasmonic nanostructures is challenging
due to strict fabrication tolerances. Here we experimentally compare
two different candidates for visible light broadband high absorptance.
The first candidate is planar thin film dual layers of Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> and aluminum (Al), while the second
structure employs ultrathin Al grating/Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> dual layers. In both cases, the absorbers yield a
measured absorptance greater than 78% in the visible. A remarkably
high-absorptance bandwidth of 120 nm was measured and associated with
the large imaginary part of Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> dielectric function. We find that the simple dual-layer planar structure
is an effective absorber in the near-infrared, but its absorptance
is less effective in the visible. However, for visible wavelengths
the grating structure can blue-shift the absorptance peak to 422 nm.
The simple geometries of the plasmonic absorbers facilitate fabrication
over large areas. It has practical applications in light harvesting,
sensing, and high-resolution color printing
Gate-Programmable Electro-Optical Addressing Array of Graphene-Coated Nanowires with Sub-10 nm Resolution
The
rapid development of highly integrated photonic circuits has been
driving electro-optic (EO) devices to increasingly compact sizes,
with the perspective of being able to control light at the nanoscale.
However, tunability with spatial resolution below 10 nm scale with
conventional approaches, such as metallic nanowires, remains a challenge.
Here, we show a graphene-coated nanowire system aiming at beam spatial
modulation at a deeply subwavelength scale. By analytically and numerically
investigating the eigenmodal properties of this system, we found that
beam power can propagate along either a swinging or a helical path
in the hybrid nanowire. In particular, the period of the swing beam
and the chirality and period of the helix beam can be flexibly controlled
by tuning the chemical potential of graphene via the gate voltage.
Significantly, due to its good modal confinement, such a beam can
be independently manipulated even in the presence of another nanowire
at a separation of 40 nm, which opens a realistic path toward gate-programmable
EO addressing or data storage with ultrahigh density (64 terabyte/ÎĽm).
At the same time, by fulfilling the phase matching condition between
the two supported guided modes operating at different wavelengths,
either a full band or band-tunable terahertz wave at the nanoscale
may be achieved by nonlinear difference frequency generation. Our
proposed hybrid nanowire system opens interesting potentials to accomplish
gate-programmable EO devices at sub-10 nm scale
Controlling Lateral Fano Interference Optical Force with Au–Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> Hybrid Nanostructure
We numerically demonstrate
that a pronounced dipole–quadrupole
(DQ) Fano resonance (FR) induced lateral force can be exerted on a
dielectric particle 80 nm in radius (<i>R</i><sub>sphere</sub> = 80 nm) that is placed 5 nm above an asymmetric bow-tie nanoantenna
array based on Au/Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> dual
layers. The DQ-FR-induced lateral force achieves a broad tuning range
in the mid-infrared region by changing the states of the Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> dielectric layer between amorphous and
crystalline and in turn pushes the nanoparticle sideways in the opposite
direction for a given wavelength. The mechanism of lateral force reversal
is revealed through optical singularity in the Poynting vector. A
thermal–electric simulation is adopted to investigate the temporal
change of the Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> film’s
temperature, which demonstrates the possibility of transiting the
Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> state by electrical heating.
Our mechanism by tailoring the DQ-FR-induced lateral force presents
clear advantages over the conventional nanoparticle manipulation techniques:
it possesses a pronounced sideways force under a low incident light
intensity of 10 mW/ÎĽm<sup>2</sup>, a fast switching time of
2.6 ÎĽs, and a large tunable wavelength range. It results in
a better freedom in flexible nanomechanical control and may provide
a new means of biomedical sensing and nano-optical conveyor belts
Beam Steering of Nonlinear Optical Vortices with Phase Gradient Plasmonic Metasurfaces
The generation of photons with spin and orbital angular
momentum
is of great importance in the fields of classical and quantum optical
communications. Recent studies show that optical vortices with on-demand
angular momentum can be realized with geometric phase-controlled metasurfaces.
However, such optical vortices have two spin-locked orbital angular
momentum states, which are difficult to distinguish in the same propagating
direction. While the beam steering of the optical vortices can be
easily realized in the linear optical regime, it remains elusive in
the nonlinear optical counterpart. Here, we propose to generate and
spatially separate the spin-locked second-harmonic vortex beams through
phase gradient plasmonic metasurfaces. Based on the concept of the
nonlinear geometric phase, the fork-type phase distributions are encoded
onto the metasurfaces by using gold meta-atoms with a threefold rotational
symmetry. Under the pumping of fundamental waves in the near-infrared
regime, the spin-locked optical vortices at second-harmonic frequency
are generated and then projected to different diffraction orders.
The proposed strategy may have important applications in high-dimensional
optical information processing
Observation and Manipulation of Visible Edge Plasmons in Bi<sub>2</sub>Te<sub>3</sub> Nanoplates
Noble
metals, like Ag and Au, are the most intensively studied
plasmonic materials in the visible range. Plasmons in semiconductors,
however, are usually believed to be in the infrared wavelength region
due to the intrinsic low carrier concentrations. Herein, we observe
the edge plasmon modes of Bi<sub>2</sub>Te<sub>3</sub>, a narrow-band
gap semiconductor, in the visible spectral range using photoemission
electron microscopy (PEEM). The Bi<sub>2</sub>Te<sub>3</sub> nanoplates
excited by 400 nm femtosecond laser pulses exhibit strong photoemission
intensities along the edges, which follow a cos<sup>4</sup> dependence
on the polarization state of incident beam. Because of the phase retardation
effect, plasmonic response along different edges can be selectively
exited. The thickness-dependent photoemission intensities exclude
the spin–orbit induced surface states as the origin of these
plasmonic modes. Instead, we propose that the interband transition-induced
nonequilibrium carriers might play a key role. Our results not only
experimentally demonstrate the possibility of visible plasmons in
semiconducting materials but also open up a new avenue for exploring
the optical properties of topological insulator materials using PEEM