4 research outputs found
Plasmonic Interference in Superstructured Metal Photonic Crystals
Surface
plasma waves (SPWs) excited by illumination of 2-dimensional
superstructured metal photonic crystals (SMPCs) are investigated with
extraordinary optical transmission (EOT). An <i>m</i> × <i>m</i> lattice of holes (<i>m</i> = 3 with the period <i>p</i> of 3 μm) fabricated in an Au film atop a GaAs substrate
(refractive index <i>n</i><sub><i>d</i></sub>),
referred to as a basis plasmonic antenna (BPA), forms an SMPC that
consists of 24 × 24 BPAs with varying spacing between BPAs, <i>d</i>. Two categories of <i>d</i> are examined: κ
= <i>d</i>/<i>p</i> = <i>i</i> (<i>i</i> an integer), where SPWs generated at each BPA interfere
constructively and κ ≠<i>i</i> (<1), where
the interference leads to drastic changes in the EOT. In the first
category, the EOT associated with the fundamental SPW wavelength, <i>T</i><sub>1</sub>, decreases with increasing κ, but has
an almost invariant peak wavelength, λ<sub>1</sub>, at ∼10.1
μm (≅<i>n</i><sub><i>d</i></sub><i>p</i>), as expected. In the second category, however, the λ<sub>1</sub> for the dominant EOT peak clearly shows a red-shift to ∼12
μm with <i>T</i><sub>1</sub> reduced to ∼0
at κ = 0.5, and <i>T</i><sub>1</sub> has a damped
oscillatory dependence on κ. The shift implies strong plasmonic
interference between BPAs that follows ∼<i>n</i><sub><i>d</i></sub><i>p</i>(<i>m</i> + κ)/<i>H</i> with the integral harmonic order of the Fourier transform
of the SMPC, <i>H</i>. This rescaling of the geometric pattern,
incommensurate to the BPA period, accompanies the EOT degraded with
the dipole deviation from individual holes that provides important
relations for the crosstalk among antennas in plasmonic circuits
Nanoscale Patterned Growth Assisted by Surface Out-Diffusion of Adatoms from Amorphous Mask Films in Molecular Beam Epitaxy
Nanoscale
patterned growth (NPG) of GaAs requires the suppression
of nucleation on the amorphous SiO<sub>2</sub> mask film, defined
on a substrate by patterning. It is determined by the Ga adatom kinetics
on SiO<sub>2</sub>, leading to desorption and surface out-diffusion
(SOD) to the area beyond the mask. Their relative contributions to
NPG are examined both theoretically and experimentally. From the rate
equation of thin-film growth, a relationship between incident Ga flux
and growth temperature for NPG is analytically derived as a function
of the lateral dimension of the SiO<sub>2</sub> mask film, <i>L</i><sub>M</sub>. In the NPG by molecular beam epitaxy, <i>L</i><sub>M</sub> is varied in the range of Ga adatom migration
length. From comparison with the model, the activation energy of a
Ga adatom for desorption, <i>E</i><sub>des</sub>, is found
to be comparable to that for surface diffusion, <i>E</i><sub>diff</sub>, on the SiO<sub>2</sub> mask. They are both in the
range of 2.7–2.9 eV, lower than the Ga desorption energy from
the GaAs substrate, confirming the validity of SOD and, as a result,
NPG. This also implies that they are not clearly distinguishable on
the amorphous surface, in contrast to crystalline surfaces, where <i>E</i><sub>diff</sub> < <i>E</i><sub>des</sub>,
which is attributed to the random fluctuations in the potential lacking
long-range order. SOD can induce an actual growth rate significantly
enhanced from the nominal rate calibrated on an unpatterned wide area
by the additional adatom diffusion flux across the substrate–mask
boundary. Its role in controlling the shape and size of the nanostructures
selectively grown on the adjacent substrate surface is addressed
Media 1: Ultrafast optical wide field microscopy
Originally published in Optics Express on 08 April 2013 (oe-21-7-8763
Nonpolar InGaN/GaN Core–Shell Single Nanowire Lasers
We report lasing from nonpolar p-i-n
InGaN/GaN multi-quantum well core–shell single-nanowire lasers
by optical pumping at room temperature. The nanowire lasers were fabricated
using a hybrid approach consisting of a top-down two-step etch process
followed by a bottom-up regrowth process, enabling precise geometrical
control and high material gain and optical confinement. The modal
gain spectra and the gain curves of the core–shell nanowire
lasers were measured using micro-photoluminescence and analyzed using
the Hakki-Paoli method. Significantly lower lasing thresholds due
to high optical gain were measured compared to previously reported
semipolar InGaN/GaN core–shell nanowires, despite significantly
shorter cavity lengths and reduced active region volume. Mode simulations
show that due to the core–shell architecture, annular-shaped
modes have higher optical confinement than solid transverse modes.
The results show the viability of this p-i-n nonpolar core–shell
nanowire architecture, previously investigated for next-generation
light-emitting diodes, as low-threshold, coherent UV–visible
nanoscale light emitters, and open a route toward monolithic, integrable,
electrically injected single-nanowire lasers operating at room temperature