26 research outputs found
Beyond the Blackbox: Explaining the Machine Learning Pre-dictions of the Optical Response of Plasmon@Semiconductor Core-Shell Nanocylinders
Cross-section images and light absorption spectrum of Plasmon@Semiconductor Core-Shell Nanocylinders</p
Enhanced Harvesting of Red Photons in Nanowire Solar Cells: Evidence of Resonance Energy Transfer
Modern excitonic solar cells efficiently harvest photons in the 350−650 nm spectral range; however, device efficiencies are typically limited by poor quantum yields for red and near-infrared photons. Using Förster-type resonance energy transfer from zinc phthalocyanine donor molecules to ruthenium polypyridine complex acceptors, we demonstrate a four-fold increase in quantum yields for red photons in dye-sensitized nanowire array solar cells. The dissolved donor and surface anchored acceptor molecules are not tethered to each other, through either a direct chemical bond or a covalent linker layer. The spatial confinement of the electrolyte imposed by the wire-to-wire spacing of the close-packed nanowire array architecture ensures that the distances between a significant fraction of donors and acceptors are within a Förster radius. The critical distance for energy transfer from an isolated donor chromophore to a self-assembled monolayer of acceptors on a plane follows the inverse fourth power instead of the inverse sixth power relation. Consequently, we observe near quantitative energy transfer efficiencies in our devices. Our results represent a new design paradigm in excitonic solar cells and show it is possible to more closely match the spectral response of the device to the AM 1.5 solar spectrum through use of electronic energy transfer
Prediction of the Active Layer Nanomorphology in Polymer Solar Cells Using Molecular Dynamics Simulation
Active layer nanomorphology is a
major factor that determines the
efficiency of bulk heterojunction polymer solar cells (PSCs). Synthesizing
diblock copolymers in which acceptor and donor materials are the constituent
blocks is the most recent method to control the structure of the active
layer. In the current work, a computational method is proposed to
predict the nanomorphology of the active layer consisting of a diblock
copolymer. Diblock copolymers have a tendency to self-organize and
form well-defined nanostructures. The shape of the structure depends
on the Flory–Huggins interaction parameter (i.e., χ),
the total degree of polymerization (<i>N</i>) and volume
fractions of the constituent blocks (φ<sub>i</sub>). In this
work, molecular dynamics (MD) simulations were used to calculate χ
parameters for two different block copolymers used in PSCs: P3HT-<i>b</i>-poly(S<sub>8</sub>A<sub>2</sub>)-C<sub>60</sub> and P3HT-<i>b</i>-poly(n-butyl acrylate-<i>stat</i>-acrylate perylene)
also known as P3HT-<i>b</i>-PPerAcr. Such calculations indicated
strong segregation of blocks into cylindrical structure for P3HT-<i>b</i>-poly(S<sub>8</sub>A<sub>2</sub>)-C<sub>60</sub> and intermediate
segregation into cylindrical structure for P3HT-<i>b</i>-PPerAcr. Experimental results of P3HT-<i>b</i>-poly(S<sub>8</sub>A<sub>2</sub>)-C<sub>60</sub> and P3HT-<i>b</i>-PTP4AP,
a diblock copolymer having very similar structure to P3HT-<i>b</i>-PPerAcr, validate our predictions
Predicting Free Energies of Exfoliation and Solvation for Graphitic Carbon Nitrides Using Machine Learning
As a metal-free and visible-light-responsive photocatalyst,
graphitic
carbon nitride (g-C3N4) has emerged as a new
research hotspot and has attracted broad attention in the field of
solar energy conversion and thin-film transistors. Liquid-phase exfoliation
(LPE) is the best-known method for the synthesis of 2D g-C3N4 nanosheets. In LPE, bulk g-C3N4 is exfoliated in a solvent via high-shear mixing or sonication in
order to produce a stable suspension of individual nanosheets. Two
parameters of importance in gauging the performance of a solvent in
LPE are the free energy required to exfoliate a unit area of layered
materials into individual sheets in the solvent (ΔGexf) and the solvation free energy per unit area of a
nanosheet (ΔGsol). While approximations
for the free energies exist, they are shown in our previous work to
be inaccurate and incapable of capturing the experimentally observed
efficacy of LPE. Molecular dynamics (MD) simulations can provide accurate
free-energy calculations, but doing so for every single solvent is
time- and resource-consuming. Herein, machine learning (ML) algorithms
are used to predict ΔGexf and ΔGsol for g-C3N4. First,
a database for ΔGexf and ΔGsol is created based on a series of MD simulations
involving 49 different solvents with distinct chemical structures
and properties. The data set also includes values of critical descriptors
for the solvents, including density, surface tension, dielectric constant,
etc. Different ML methods are compared, accompanied by descriptor
selection, to develop the most accurate model for predicting ΔGexf and ΔGsol. The extra tree regressor is shown to be the best performer among
the six ML methods studied. Experimental validation of the model is
conducted by performing dispersibility tests in several solvents for
which the free energies are predicted. Finally, the influence of the
selected descriptors on the free energies is analyzed, and strategies
for solvent selection in LPE are proposed
Anodic Growth of Large-Diameter Multipodal TiO<sub>2</sub> Nanotubes
We report on the formation of a new class of nanostructures, namely, multipodal hollow titania nanotubes possessing two or more legs, achieved during the electrochemical anodization of titanium in diethylene glycol (DEG)-based electrolytes. The unique multipodal porous structure is expected to extend and enhance the applications of TiO2 nanotube arrays. Multipodal nanotubes form by a process we term “nanotube combination”, which only occurs in viscous electrolytes at high anodization potentials in the presence of a low concentration of fluoride-bearing species. The mechanism of formation of multipodal nanotubes is considered, and the tube length at which nanotube combination occurs is predicted theoretically using a simplified analytical model. The results suggest that capillary forces strong enough to bend the TiO2 nanotubes by tens of degrees are generated during the imbibition of electrolyte into and out of the intertubular spaces between adjacent tapered nanotubes
Distinguishing between Deep Trapping Transients of Electrons and Holes in TiO<sub>2</sub> Nanotube Arrays Using Planar Microwave Resonator Sensor
A large
signal direct current (DC) bias and a small signal microwave
bias were simultaneously applied to TiO2 nanotube membranes
mounted on a planar microwave resonator. The DC bias modulated the
electron concentration in the TiO2 nanotubes and was varied
between 0 and 120 V in this study. Transients immediately following
the application and removal of DC bias were measured by monitoring
the S-parameters of the resonator as a function of
time. The DC bias stimulated Poole–Frenkel-type trap-mediated
electrical injection of excess carriers into TiO2 nanotubes,
which resulted in a near-constant resonant frequency but a pronounced
decrease in the microwave amplitude due to free electron absorption.
When ultraviolet illumination and DC bias were both present and then
stepwise removed, the resonant frequency shifted due to trapping-mediated
change in the dielectric constant of the nanotube membranes. Characteristic
lifetimes of 60–80, 300–800, and ∼3000 s were
present regardless of whether light or bias was applied and were also
observed in the presence of a hole scavenger, which we attributed
to oxygen adsorption and deep electron traps, whereas another characteristic
lifetime >8000 s was only present when illumination was applied,
and
is attributed to the presence of hole traps
Dimension-Controlled Synthesis of Hybrid-Mixed Halide Perovskites for Solar Cell Application
Despite
the rapid improvement of photovoltaic (PV) efficiency
in
hybrid organic–inorganic metal halide perovskites (HOIPs),
the fabrication procedure of a compact thin film in a large-area application
is still a tedious work. Apart from the quality of the thin film,
the stability of the perovskite materials and the expensive organic
hole transport layer (HTL) within the HOIP-based PV device are the
major issues that need to be addressed prior to their commercialization.
Herein, a unique glass rod-based facile fabrication technique for
producing a compact and stable thin film utilizing a mixed-halide-based
perovskite precursor solution is demonstrated. The fabricated devices
deliver high photoconversion efficiency (PCE) without the use of any
HTL and show an excellent stability under ambient conditions. By varying
the organic CH3NH3I (MAI) and inorganic PbBr2 content, perovskite materials with different dimensions,
i.e., 3D, 2D, and 1D, are synthesized to produce an active layer for
PV devices. Although a 2D single-halide perovskite is reported earlier,
herein two different mixed-halide 2D perovskites, i.e., MA2PbI2Br2 and MAPb2IBr4, are synthesized successfully, and their performance is compared
in detail along with that of 1D and 3D mixed-halide perovskites. The
facile synthesized mixed-halide 2D-based MA2PbI2Br2 perovskite shows a PCE of 10.14% with a high stability
of 92% after 100 days without encapsulation, which is much superior
as compared to that of the mixed-halide 3D MAPbIBr2. The
semiconducting behavior as well as the nature of the bandgap of the
synthesized compounds is examined by pursuing density functional theory
calculations. Specifically, the role of iodine doping to modify the
electronic band structure is investigated, and introduction of iodine
is found to reduce the effective masses of both electrons and holes
in the perovskite material
High Breakdown Strength Schottky Diodes Made from Electrodeposited ZnO for Power Electronics Applications
The
synthesis of ZnO films by optimized electrodeposition led to the achievement
of a critical electric field of 800 kV/cm. This value, which is 2–3
times higher than in monocrystalline silicon, was derived from a vertical
Schottky diode application of columnar-structured ZnO films electrodeposited
on platinum. The device exhibited a free carrier concentration of
2.5 × 1015 cm–3, a rectification
ratio of 3 × 108, and an ideality factor of 1.10,
a value uncommonly obtained in solution-processed ZnO. High breakdown
strength and high thickness capability make this environment-friendly
process a serious option for power electronics and energy harvesting
Multinuclear Magnetic Resonance Tracking of Hydro, Thermal, and Hydrothermal Decomposition of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>
An NMR investigation
of methylammonium lead iodide, the leading
member of the hybrid organic–inorganic perovskite class of
materials, and of its putative decomposition products as a result
of exposure to heat and humidity, has been undertaken. We show that
the <sup>207</sup>Pb NMR spectra of the compound of interest and of
the proposed lead-containing decomposition products, CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>·H<sub>2</sub>O, (CH<sub>3</sub>NH<sub>3</sub>)<sub>4</sub>PbI<sub>6</sub>·2H<sub>2</sub>O,
and PbI<sub>2</sub>, have distinctive chemical shifts spanning over
1400 ppm, making <sup>207</sup>Pb NMR an ideal tool for investigating
this material; further information may be gained from <sup>13</sup>C and <sup>1</sup>H NMR spectra. As reported in many investigations
of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> on films, the bulk
material hydrates in the presence of high relative humidity (approximately
80%), yielding the monohydrated perovskite CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>·H<sub>2</sub>O. This reaction is reversible
by heating the sample to 341 K. We show that neither (CH<sub>3</sub>NH<sub>3</sub>)<sub>4</sub>PbI<sub>6</sub>·2H<sub>2</sub>O nor
PbI<sub>2</sub> is observed as a decomposition product and that, in
contrast to many studies on CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> films, the bulk material does not decompose or degrade beyond CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>·H<sub>2</sub>O upon prolonged
exposure to humidity at ambient temperature. However, exposing CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> concurrently to heat and humidity,
or directly exposing it to liquid water, leads to the irreversible
formation of PbI<sub>2</sub>. In spite of its absence among the decomposition
products, the response of (CH<sub>3</sub>NH<sub>3</sub>)<sub>4</sub>PbI<sub>6</sub>·2H<sub>2</sub>O to heat was also investigated.
It is stable at temperatures below 336 K but then rapidly dehydrates,
first to CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>·H<sub>2</sub>O and then to CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>. The higher
stability of the bulk material as reported here is a promising advance,
since stability is a major concern in the development of commercial
applications for this material
Vertically Aligned Single Crystal TiO<sub>2</sub> Nanowire Arrays Grown Directly on Transparent Conducting Oxide Coated Glass: Synthesis Details and Applications
Single-crystal one-dimensional (1D) semiconductor architectures are important in materials-based applications requiring a large surface area, morphological control, and superior charge transport. Titania has widespread utility in applications including photocatalysis, photochromism, photovoltaics, and gas sensors. While considerable efforts have focused on the preparation of 1D TiO2, no methods have been available to grow crystalline nanowire arrays directly onto transparent conducting oxide (TCO) substrates, greatly limiting the performance of TiO2 photoelectrochemical devices. Herein, we present a straightforward low temperature method to prepare single crystal rutile TiO2 nanowire arrays up to 5 μm long on TCO glass via a non-polar solvent/hydrophilic substrate interfacial reaction under mild hydrothermal conditions. The as-prepared densely packed nanowires grow vertically oriented from the TCO glass substrate along the (110) crystal plane with a preferred (001) orientation. In a dye sensitized solar cell, N719 dye, using TiO2 nanowire arrays 2−3 μm long we achieve an AM 1.5 photoconversion efficiency of 5.02%
