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This PDF file contains the front matter associated with SPIE
Proceedings Volume 7764, including the Title Page, Copyright
information, Table of Contents, and the Conference Committee listing.
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In an effort to engineer photonic crystal slab (PCS) devices that operate within a single slab-mode regime, the
effect of increased cladding index was studied using FDTD simulation. It is known that while increased cladding
index forces the light-cone to constrict in frequency, the single mode condition eases allowing for the use of
thicker slabs that remain single-mode. This study shows that the behavior of the photonic band gap is similar to
that of the light-cone, sweeping lower in frequency, and even widening in some cases, as cladding index
increases. Band gap behavior for both even and odd polarizations over thicknesses from d/a = 0.2 to 0.6 and
cladding indices from 1 to 2.5 were studied in efforts to design a single-mode, polarization insensitive, complete
band gap. When graphically overlaid, the light-cone, single-mode condition, and transmission spectra represent
an enabling reference for the design of realizable structures. For device applications where modal dispersion is
detrimental or single mode operation is necessary, a paradigm shift away from air-bridge devices is shown to be
essential as single-mode structures of this type demand slab thicknesses far too thin for adequate band gap engineering.
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Polymer-based flexible Cu stripe optical waveguides have been developed to configure a board-level optical
interconnection. By embedding Cu stripe in a dual slab waveguide with high refractive-index contrast, the field of the
guided mode is confined more in the two dielectric core layers. Thus, significant reduction of the propagation and
vertical bending loss are expected. The fabricated Cu plasmonic waveguide is flexible enough to be bent down to a
radius of 0.5 mm. The measured optical properties are satisfactory for very short distance board-level optical
interconnection. Based on the experimental results, we concluded that hybrid Cu plasmonic waveguides have a great
potential to be developed as a means of optical signal guiding medium in the optical interconnections.
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A polarization-independent racetrack type micro-ring resonator formed by silicon-on-insulator slot waveguides with a
phase compensation section included was investigated and proposed. By tuning the ratio of lengths of the slot waveguide
and the channel waveguide the cumulative phase difference between quasi-TE and quasi-TM modes can be well
eliminated which allows for a polarization independent operation over a wide spectral range. The finesses are 226 and
225 for the quasi-TE and quasi-TM modes respectively, with a free spectral range of 9 nm achieved as well as a compact
device size of 30 μm, while delivering a good polarization-independent performance with the resonance mode mismatch
less than 0.5 nm.
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Energy Conversion and Alternative Energy Solutions Through Nanoengineering
We describe nanotechnologies used to improve the efficient harvest of energy from the Sun and the wind, and the
efficient storage of energy in secondary batteries and ultracapacitors, for use in a variety of applications including smart
grids, electric vehicles, and portable electronics.
We demonstrate high-quality nanostructured copper indium gallium selenide (CIGS) thin films for photovoltaic (PV)
applications. The self-assembly of nanoscale p-n junction networks creates n-type networks that act as preferential
electron pathways, and p-type networks that act as preferential hole pathways, allowing positive and negative charges to
travel to the contacts in physically separated paths, reducing charge recombination. We also describe PV
nanotechnologies used to enhance light trapping, photon absorption, charge generation, charge transport, and current
collection.
Furthermore, we describe nanotechnologies used to improve the efficiency of power-generating wind turbines. These
technologies include nanoparticle-containing lubricants that reduce the friction generated from the rotation of the
turbines, nanocoatings for de-icing and self-cleaning technologies, and advanced nanocomposites that provide lighter
and stronger wind blades.
Finally, we describe nanotechnologies used in advanced secondary batteries and ultracapacitors. Nanostructured
powder-based and carbon-nanotube-based cathodes and anodes with ultra-high surface areas boost the energy and power
densities in secondary batteries, including lithium-ion and sodium-sulfur batteries. Nanostructured carbon materials are
also controlled on a molecular level to offer large surface areas for the electrodes of ultracapacitors, allowing to store
and supply large bursts of energy needed in some applications.
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We report the results of fabrication and testing of a thermoelectric power generation module. The
module was fabricated using a new "flip-chip" module assembly technique that is scalable and
modular. This technique results in a low value of contact resistivity ( ≤ 105 Ω-cm2 ). It can be used to leverage new advances in thin-film and nanostructured materials for the fabrication of new
miniature thermoelectric devices. It may also enable monolithic integration of large devices or tandem arrays of devices on flexible or curved surfaces. Under mild testing, a power of 22 mW/cm2 was obtained from small (<100 K) temperature differences. At higher, more realistic temperature differences, ~500 K, where the efficiency of these materials greatly improves, this power density would scale to between 0.5 and 1 Watt/cm2. These results highlight the excellent potential for the generation and scavenging of electrical power of practical and usable magnitude for remote applications using thermoelectric power generation technologies.
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We study the coupled electro-mechanical effects in the band structure calculations of low dimensional semiconductor
nanostructures (LDSNs) such as AlN/GaN quantum dots. Some effects in these systems are essentially
nonlinear. Strain, piezoelectric effects, eigenvalues and wave functions of a quantum dot have been used as
tuning parameters for the optical response of LDSNs in photonics, band gap engineering and other applications. However, with a few noticeable exceptions, the influence of piezoelectric effects in the electron wave functions
in Quantum Dots (QDs) studied with fully coupled models has been largely neglected in the literature. In this paper, by using the fully coupled model of electroelasticity, we analyze the piezoelectric effects into the band structure of cylindrical quantum dots. Results are reported for III-V type semiconductors with a major focus given to AlN/GaN based QD systems.
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In this paper we demonstrate how an elliptically shaped semiconductor microcavity can be used to generate surface
plasmons (SP) mode by pumping current and injecting optical pulse. After achieving stable lasing mode, external
magnetic field is applied to a small elliptical confined area on the elliptical microcavity. The applied magnetic field
produces Lorentz torque and "pushes" the electrons to the edge of the microcavity. Strong electron plasma is built up on
the boundary of the microcavity and air interface as more electrons accumulate. The laser light source interacts with the
electron plasma at the boundary of microcavity and excites surface plasmon mode. The direct excitation of SPP modes
could be used to extract the laser light from elliptical microcavity source and results in a lower coupling loss and higher
efficient small coupling system.
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Direct writing using a femtosecond laser provides an accurate, repeatable and efficient means of creating
nanoscale lines for electronic applications circumventing the standard fabrication methods that require
expensive masks and numerous processing steps. Femtosecond laser writing makes these nanoscale lines by
using a phase zone plate to focus the laser pulse onto a silicon substrate in a chemical vapor deposition
chamber flowing silane. The silane is decomposed onto the narrow heated area of the substrate as the laser
scans across leaving behind a thin line of silicon deposition. This manufacturing technique utilizes a high
precision optical metrology system and a high precision motion control system to make this nanomanufacturing
possible. It has been shown to successfully make as many as 100 silicon lines on the order of a few hundred nanometers in width. The size and crystal structure of these lines are characterized using Scanning Electron Microscopy (SEM) and Transmission Electron Microscopy (TEM).
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Thin, free-standing boro-phosphosilicate glass (BPSG) films (<1.5 μm thick, 10 - 20 mm2) were fabricated (PSU NSF -
NNIN Site) to serve as neutron converting media for a proposed high-resolution neutron imaging system capable of submicron
sample imaging . The B and P concentration in the BPSG films was 4.5 and 3.5 w%, respectively, measured by
ICP-OES. Silicon nitride (Si3N4) was deposited on both sides of the wafer to act as an etch mask and a protective layer over the BPSG. The bulk wafer stress induced by the lower expansion Si3N4 and BPSG layers was ~90 MPa (tensile). The Si substrate was removed from the photolithography-patterned areas via wet etch in KOH:DI H2O (45:55) solution
at 100°C so that the exposed areas consisted of free-standing Si3N4/BPSG/Si3N4 stacked windows. The Si3N4 was removed via MERIE from the windows. NDP of the processed films showed that the boron concentration was constant
and uniform throughout the exposed BPSG film. Visual observations of the free-standing windows showed long-range
spatial deformation of the films in terms of "waves" caused by stress gradients, which were observed near the edges of
the windows using optical birefringence. An annealing schedule was implemented to determine if the glass film
deformation was caused by residual stress in the as-deposited film. Preliminary results of these experiments imply
another mechanism is responsible for the deformation of the free-standing films. This work will review the processing
techniques used in film fabrication and present the results of the thermal treatments of the thin, free-standing BPSG films.
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Nanofabrication: New Techniques, Properties, and Emerging Applications
Logic gates consisting of DNA molecules are useful for direct processing of information that relates to biomolecules
including DNA at nanoscale. This study is aimed at demonstrating operation of the DNA logic gates by optical
manipulation of micro-droplets that contain DNA to show potential of photonics techniques in realizing nanoscale
computing. Connections of different DNA logic gates are reconfigurable owing to flexibility in manipulating the
micro-droplets. The method is effective in, for example, implementing logic operations in limited-volumes at
multiple positions in parallel, enhancing an operation rate, and decreasing sample consumption, and it can be a
promising technique applicable to photonic DNA computing.
We used a two-input and one-output AND or OR gate consisting of DNA in experiments. The individual
inputs, A and B, were encoded into different DNA molecules, I1 and I2, and the output was obtained from a
fluorescence signal. Input A (B) is 1 when DNA I1 (I2) exists, and 0 when the DNA does not exist. Microdroplets were made by mixing DNA solution, acetophenone as solvent, and sorbitan monooleate as surfactant. For
AND/OR operation, two micro-droplets, one of which contained input-DNAs and the other contained AND/OR
logic gates, were optically manipulated to be in contact each other; then the micro-droplets coalesced and the
operation started. Experimental results show that expected fluorescence intensities are obtained as the output
for all possible input values, and logic operation can be implemented successfully in optically manipulated microdroplets.
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A nanoimprinted polymer chip with a thin near-infrared absorber layer that enables light-induced local heating (LILH)
of liquids inside micro- and nanochannels is presented. An infrared laser spot and corresponding hot-spot could be
scanned across the device. Large temperature gradients yield thermophoretic forces, which are used to manipulate and
stretch individual DNA molecules confined in nanochannels. The absorber layer consists of a commercially available
phthalocyanine dye (Fujifilm), with a narrow absorption peak at approximately 775 nm, dissolved in SU-8 photoresist
(Microchem Corp.). The 500 nm thick absorber layer is spin-coated on a transparent substrate and UV exposed. Microand
nanofluidic channels are defined by nanoimprint lithography in a 1.5 μm thick layer of low molecular weight
polymethyl methacrylate (PMMA, Microchem Corp.), which is spin coated on top of the absorber layer. We have used a
previously developed two-level hybrid stamp for replicating two V-shaped microchannels (width=50 μm and height =
900 nm) bridged by an array of 200 nanochannels (width and height of 250 nm). The fluidic channels are finally sealed
with a lid using PMMA to PMMA thermal bonding. Light from a 785 nm laser diode was focused from the backside of
the chip to a spot diameter down to 5 ..m in the absorber layer, yielding a localized heating (Gaussian profile) and large
temperature gradients in the liquid in the nanochannels. A laser power of 38 mW yielded a temperature of 40oC in the
center of a 10 μm 1/e diameter. Flourescence microscopy was performed from the frontside.
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Nanoporous liquid core waveguides are fabricated by selectively UV modifying a nanoporous polymer. The
starting point is a diblock polymer where 1,2-polybutadiene (PB) molecules are bound to PDMS. When the PB
is cross linked it self-assembles into PB with a network of 14 nm diameter PDMS filled pores. When the PDMS
is etched, the hydrophobic PB is left with a porosity of 44%. The polymer is subsequently UV exposed through
a shadow mask. This renders the exposed part hydrophilic, making it possible for water to infiltrate these areas.
Water infiltration raises the refractive index, thus forming a liquid core waveguide. Here we present both the
fabrication scheme and characterization results for the waveguides.
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A new nanoscale electric field sensor was developed for studying triboelectric charging in
terrestrial and Martian dust devils. This sensor is capable to measure the large electric fields for
large dust devils without saturation. However, to quantify the electric charges and the field
strength it is critical to calibrate the mechanical stiffness of the sensor devices. We performed a
technical feasibility study of the Nano E-field Sensor stiffness by a non-contact stiffness
measurement method. The measurement is based on laser Doppler vibrometer measurement of
the thermal noise due to energy flunctuations in the devices. The experiment method provides a
novel approach to acquire data that is essential in analyzing the quantitative performance of the
E-field Nano Sensor. To carry out the non-contact stiffness measurement, we fabricated a new
Single-Walled Carbon Nanotube (SWCNT) E-field sensor with different SWCNTs suspension
conditions. The power spectra of the thermal induced displacement in the nano E-field sensor
were measured at the accuracy of picometer. The power spectra were then used to derive the
mechanical stiffness of the sensors. Effect of suspension conditions on stiffness and sensor
sensitivty was discussed. After combined deformation and resistivity measurement, we can
compare with our laboratory testing and field testing results. This new non-contact measurement
technology can also help to explore to other nano and MEMS devices in the future.
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Para-hexaphenylene (p6P) molecules have the ability to self-assemble into organic nanofibers, which exhibit a
range of interesting optical and optoelectronic properties such as intense, polarized luminescence, waveguiding and
lasing. The nanofibers are typically grown on specific single-crystalline templates, such as muscovite mica, on which
mutually parallel nanofibers are self-assembled upon vapor deposition of the organic material under high vacuum
conditions. Besides such single-crystalline templates, the nanofibers can also be grown on non-crystalline gold
surfaces, on which the orientation of the nanofibers can be manipulated by structuring the gold surface prior to parahexaphenylene
(p6P) deposition. In this work it is demonstrated, how such organic nanofiber growth can be controlled
by modifying the design of the underlying gold structures prior to growth. Here, the investigated designs include
pinning lines and gratings. We demonstrate how gold gratings fabricated on an insulating substrate can enable
electrical contact to in-situ grown p6P nanofibers. Furthermore, the electrical characteristics of in-situ grown fibers are compared to that of transferred p6P nanofibers. The transferred nanofibers are initially grown on muscovite mica, and
subsequently transferred onto a target substrate by drop casting, and electrodes are applied on top by a special shadow
mask technique.
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Surface Enhanced Raman Scattering (SERS) is a recently discovered powerful technique which has demonstrated
sensitivity and selectivity for detecting single molecules of certain chemical species. This is due to an enhancement
of Raman scattered light by factors as large as 1015. Gold and Silver-coated substrates fabricated by electron-beam
lithography on Silicon are widely used in SERS technique. In this paper, we report the use of nanoporous ceramic
membranes for SERS studies. Nanoporous membranes are widely used as a separation membrane in medical
devices, fuel cells and other studies. Three different pore diameter sizes of commercially available nanoporous
ceramic membranes: 35 nm, 55nm and 80nm are used in the study. To make the membranes SERS active, they are
coated with gold/silver using sputtering techniques. We have seen that the membranes coated with gold layer remain
unaffected even when immersed in water for several days. The results show that gold coated nanoporous membranes
have sensitivity comparable to substrates fabricated by electron-beam lithography on Silicon substrates.
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In order for laser oscillation to occur, the modal gain at the lasing photon energy must equal the total losses. In this work,
we analyze and calculate the total losses due to the free carrier absorption, optical waveguide scattering and the laser
cavity end losses for PbSe/Pb0.934Sr0.066 Se quantum well laser structures. The small confinement factor value causes the free carrier absorption loss to be negligible. The calculated scattering loss values showed a decreasing order for the
MQW, MMQW and SCH-SQW structures, for a surface roughness amplitude of 10nm. Increasing the surface roughness
amplitude increases these scattering losses even further. However, the calculated cavity loss calculations showed that its
values are in an increasing order for the MQW (or MMQW) and SCH-SQW structures. These cavity losses are lowest
for uncoated cavity ends. Coating these ends with a quarter wavelength BaF2 layer increases the total cavity loss. In
addition, coating the cavity ends with alternating quarter wavelength layers of BaF2 and CaF2 also results in an increase in the cavity loss. The increase in cavity loss due to coating is caused by the decrease in the mirrors' reflectivity values. These results show that coating with fluoride layers can best be utilized in applications where high transitivity values are needed.
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The aim of present paper is to present the latest results on investigations of the carbon thin film deposited by
Thermionic Vacuum Arc (TVA) method and laser pyrolysis. X-ray photoelectron spectroscopy (XPS) and X-ray generated Auger electron spectroscopy (XAES) were used to determine composition and sp2 to sp3 ratios in the outer
layers of the film surfaces. The analyses were conducted in a Thermoelectron ESCALAB 250 electron spectrometer
equipped with a hemispherical sector energy analyser. Monochromated Al K X-radiation was employed for the XPS
examination, at source excitation energy of 15 KeV and emission current of 20 mA. Analyzer pass energy of 20 eV with
step size of 0.1 eV and dwell time of 100 ms was used throughout.
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Glass surface roughness with defined morphologies is realized by a two step lithography-free process: first sputter deposition
of an around 10 nm thin unstructured metallic layer onto the surface, second reactive ion etching in an Ar/CF4 high
density plasma. During the etch step metal atoms and etch gas constituents build hardly volatile metal halogen compounds
resulting in self-masking of the glass. Several metals like Ag, Al, Au, Cu, In, and Ni can be employed as the
metallic seed layer in this technology. Within the second process step the sacrificial metal layer is completely removed
from the surface. Due to the locally varying etch velocity further etching causes formation of pits and elevations with
typical height and lateral dimensions on the order of 0.5 μm. Surface morphology is influenced by choice of seed layer
material and etch parameters, resulting in a multitude of different morphologies. Hence optical scattering characteristics
of the glass can be tuned almost arbitrarily over a wide range. The dosed extents of light scattering could possibly be
used advantageously for specific classes of applications, e.g. lighting engineering, efficiency enhancement of thin film
solar cells or organic light emitting diodes.
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We investigate commercial nano-engineered SERS (surface enhanced Raman spectroscopy) substrates for the
possibility of recycling them and using them multiple times. KlariteTM is a commercial SERS substrate fabricated by
nanoscale lithographic patterning technique on silicon wafer before being coated with a thin layer of Gold. It has
been widely reported that, this substrate results in more reproducible surface enhanced Raman signals. However, it
is designed only for a single measurement and disposable use. In this work, we report a method for recycling one
substrate for multiple SERS measurements by coating a thin layer of Gold/Silver after each application of the
substrate. The results obtained using reprocessed substrates are comparable to the measurements recorded using fresh substrates.
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We present the first results of fabrication the circular zone plate by means of high resolution negative tone inorganic
HSQ (Hydrogen Silsesquioxane or XR-1541) electron-beam resist. Fresnel zone plates (FZPs) has been fabricated on the
surface of silicon crystals for the energy from 8keV up to 100keV by electron beam lithography. Three different FZPs
have been fabricated; circular FZP for the first diffraction order, circular compound FZP for the first and third diffraction
order, and linear FZP for the first and second diffraction order. The parameters of the compound FZPs for first and third
order were the following: the focal distance of first and third orders FZP is F =13.229cm for 0.1nm wavelength, the
entire aperture is 400.0016μm, the width of the outermost zones of the first and third orders is 100nm, and the number of
the first and third order zones is 1223.
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We apply the former general dynamical model of drying process of polymer solution coated on a flat
substrate for flat polymer film fabrication to concrete detailed subjects. Concretely we apply the model to
effects of a bumpy substrate as an example. We understand that a humpy structure on a substrate does not
affect nearly solute's distribution after drying because effects of diffusion around the hump are sufficiently
effective as far as the hump interfere with diffusion. We also understand that when the beginning time of
special vaporization near a hump is earlier, solute's distribution after drying except for at the edge's region is
thinner a little because leveling including the edge's region by diffusion is more effective.
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Fiber optic sensor is proposed based on cladding modification method for detecting ammonia emissions. Nanocrystalline titanium dioxide is used as a sensing material and spectral characteristics of the
sensor are studied for different concentrations (50-500 ppm) of ammonia, methanol and ethanol. The sensor
shows a linear variation in the output light intensity with the concentration. The light intensity increases for
ammonia whereas it decreases for methanol and ethanol. Gas selectivity of the sensor is discussed.
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Zinc Oxide nanostructures are capable of applying numerous applications such as optoelectronics, sensors, varistors,
and electronic devices. There are several techniques to gorw ZnO nanostructures, including vapor-liquid-solid method,
chemical vapor deposition, physical vapor deposition, metal organic chemical vapor deposition and solution process.
Recently reported solution method is a simple way to grow ZnO nanowires at a low temperature. One distinctive
advantage with the solution method is low processing temperature so that flexible polymer materials can be used as a
substrate to grow ZnO nanowires. In this study, ZnO nanowires have been fabricated on PET film by solution method
with various molarities to see the effect of different molarities on ZnO nanowire growth. The solution temperature was
80°C and ZnO nanowires were grown for 6 hours for each case. The ZnO seed layer was sputtered at room temperature
for 33 min. prior to ZnO nanowire growth. These ZnO nanowires were characterized by X-ray diffraction (XRD),
Scanning Electron Microscopy (SEM), and photoluminescence (PL) measurements at room temperature using a He-Cd
325-nm laser as the excitation source. We also measured the current using current Atomic Force Microscopy (I-AFM)
and presented the possibility to use ZnO nanowires as a power source for micro/nano scale devices. As a result, we found
that the characterization of ZnO nanowires changes according to the solution molarity.
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Bending efficiency of three-dimensional (3-D) horizontal single- and multiple-slot waveguide microrings are analyzed
using a combination of effective-index and modified transfer-matrix methods. The effects of waveguide parameters,
low-index material, high-index material, asymmetric structure, and asymmetric slots on the bending loss are studied. We
show that the bending efficiency can be enhanced by applying asymmetric structures and asymmetric slots. In addition,
it is demonstrated that the bending loss increases with increasing the number of slots. However, by using proper
thicknesses for different high-index layers of horizontal multiple-slot waveguide, it is possible that horizontal multipleslot
waveguide can provide a lower bending loss than the single-slot one.
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