69 research outputs found
Bilayer Phosphorene: Effect of Stacking Order on Bandgap and Its Potential Applications in Thin-Film Solar Cells
Phosphorene, a monolayer
of black phosphorus, is promising for
nanoelectronic applications not only because it is a natural p-type
semiconductor but also because it possesses a layer-number-dependent
direct bandgap (in the range of 0.3 to 1.5 eV). On basis of the density
functional theory calculations, we investigate electronic properties
of the bilayer phosphorene with different stacking orders. We find
that the direct bandgap of the bilayers can vary from 0.78 to 1.04
eV with three different stacking orders. In addition, a vertical electric
field can further reduce the bandgap to 0.56 eV (at the field strength
0.5 V/Ć
). More importantly, we find that when a monolayer of
MoS<sub>2</sub> is superimposed with the p-type AA- or AB-stacked
bilayer phosphorene, the combined trilayer can be an effective solar-cell
material with type-II heterojunction alignment. The power conversion
efficiency is predicted to be ā¼18 or 16% with AA- or AB-stacked
bilayer phosphorene, higher than reported efficiencies of the state-of-the-art
trilayer graphene/transition metal dichalcogenide solar cells
Electron-Transport Properties of Few-Layer Black Phosphorus
We
perform the first-principles computational study of the effect
of number of stacking layers and stacking style of the few-layer black
phosphorus (BPs) on the electronic properties, including transport
gap, currentāvoltage (<i>i</i>ā<i>v</i>) relation, and differential conductance. Our computation is based
on the nonequilibrium Greenās function approach combined with
density functional theory calculations. Specifically, we compute electron-transport
properties of monolayer BP, bilayer BP, and trilayer BP as well as
bilayer BPs with AB-, AA-, or AC-stacking. We find that the stacking
number has greater influence on the transport gap than the stacking
type. Conversely, the stacking type has greater influence on <i>i</i>ā<i>v</i> curve and differential conductance
than on the transport gap. This study offers useful guidance for determining
the number of stacking layers and the stacking style of few-layer
BP sheets in future experimental measurements and for potential applications
in nanoelectronic devices
Al<sub>2</sub>C Monolayer Sheet and Nanoribbons with Unique Direction-Dependent Acoustic-Phonon-Limited Carrier Mobility and Carrier Polarity
The intrinsic acoustic-phonon-limited
carrier mobility (Ī¼)
of Al<sub>2</sub>C monolayer sheet and nanoribbons are investigated
using ab initio computation and deformation potential theory. It is
found that the polarity of the room-temperature carrier mobility of
the Al<sub>2</sub>C monolayer is direction-dependent, with Ī¼
of electron (<i>e</i>) and hole (<i>h</i>) being
2348 and 40.77 cm<sup>2</sup>/V/s, respectively, in the armchair direction
and 59.95 (<i>e</i>) and 705.8 (<i>h</i>) in the
zigzag direction. More interestingly, one-dimensional Al<sub>2</sub>C nanoribbons not only can retain the direction-dependent polarity
but also may entail even higher mobility, in contrast to either the
graphene nanoribbons which tend to exhibit lower Ī¼ compared
to the two-dimensional graphene or the MoS<sub>2</sub> nanoribbons
which have reversed polarity compared to the MoS<sub>2</sub> sheet.
As an example, the Al-terminated zigzag nanoribbon with a width of
4.1 nm exhibits Ī¼ of 212.6 (<i>e</i>) and 2087 (<i>h</i>) cm<sup>2</sup>/V/s, while the C-terminated armchair nanoribbon
with a width 2.6 nm exhibits Ī¼ of 1090 (<i>e</i>)
and 673.9 (<i>h</i>) cm<sup>2</sup>/V/s; the C-terminated
zigzag nanoribbon with a width 3.7 nm exhibits Ī¼ of 177.6 (<i>e</i>) and 1889 (<i>h</i>) cm<sup>2</sup>/V/s, and
the Al-terminated armchair nanoribbon with a width 2.4 nm exhibits
Ī¼ of 6695 (<i>e</i>) and 518.4 (<i>h</i>) cm<sup>2</sup>/V/s. The high carrier mobility, Ī¼, coupled
with polarity and direction dependence endows the Al<sub>2</sub>C
sheet and nanoribbons with unique transport properties that can be
exploited for special applications in nanoelectronics
Fluorescence of A100 MOF and Adsorption of Water, Indole, and Naphthalene on A100 by the Spectroscopic, Kinetic, and DFT Studies
Metalāorganic
frameworks (MOFs) are promising materials
for adsorption and separations. It is important to understand the
details of chemical bonding between the adsorbate and structural units
in the MOFs. In A100 MOF, the near-UVāvisible fluorescence
is found to be the intralinker fluorescence. Naphthalene and indole
form the stoichiometric āhost-guestā ĻāĻ
adsorption complexes with A100 that contain one adsorbate molecule
per two BDC linkers, and adsorption of indole causes a strong quenching
of the intralinker fluorescence. The excitation wavelength dependent
steady-state fluorescence spectra, the nanosecond time-resolved fluorescence
spectra, and DFT calculations indicate the strong ĻāĻ
interactions between adsorbed indole and naphthalene and aromatic
ring of the BDC linker, as well as hydrogen bonding between adsorbed
indole and COO group of the linker. Activated A100 adsorbs up to four
water molecules per BDC linker. Kinetic study of adsorption of naphthalene
and indole from <i>n</i>-alkane on hydrated A100 yields
the preferential adsorption of indole as determined by the in-situ
time-dependent fluorescence spectroscopy and complementary ex-situ
UVāvis absorption spectroscopy
Capillary Isoelectric Focusing-Mass Spectrometry Method for the Separation and Online Characterization of Intact Monoclonal Antibody Charge Variants
We report a new online
capillary isoelectric focusing-mass spectrometry
(CIEF-MS) method for monoclonal antibody (mAb) charge variant analysis
using an electrokinetically pumped sheath-flow nanospray ion source
and a time-of-flight MS with pressure-assisted chemical mobilization.
To develop a successful, reliable CIEF-MS method for mAb, we have
selected and optimized many critical, interrelating reagents and parameters
that include (1) MS-friendly anolyte and catholyte; (2) a glycerol
enhanced sample mixture that reduced non-CIEF electrophoretic mobility
and band broadening; (3) ampholyte selected for balancing resolution
and MS sensitivity; (4) sheath liquid composition optimized for efficient
focusing, mobilization, and electrospray ionization; (5) judiciously
selected CIEF running parameters including injection amount, field
strength, and applied pressure. The fundamental premise of CIEF was
well maintained as verified by the linear correlation (<i>R</i><sup>2</sup> = 0.99) between p<i>I</i> values and migration
time using a mixture of p<i>I</i> markers. In addition,
the charge variant profiles of trastuzumab, bevacizumab, infliximab,
and cetuximab, obtained using this CIEF-MS method, were corroborated
by imaged CIEF-UV (iCIEF-UV) analyses. The relative standard deviations
(RSD) of absolute migration time of p<i>I</i> markers were
all less than 5% (<i>n</i> = 4). Triplicate analyses of
bevacizumab showed RSD less than 1% for relative migration time to
an internal standard and RSD of 7% for absolute MS peak area. Moreover,
the antibody charge variants were characterized using the online intact
MS data. To the best of our knowledge, this is the first time that
direct online MS detection and characterization were achieved for
mAb charge variants resolved by CIEF as indicated by a well-established
linear pH gradient and correlated CIEF-UV charge variant profiles
Efficient Visible-Light-Driven Photocatalytic Degradation with Bi<sub>2</sub>O<sub>3</sub> Coupling Silica Doped TiO<sub>2</sub>
A new
TiO<sub>2</sub>-based visible light photocatalyst (Bi<sub>2</sub>O<sub>3</sub>/SiāTiO<sub>2</sub>) was synthesized by
both Bi<sub>2</sub>O<sub>3</sub> coupling and Si doping via a two-step
method. The structural, morphological, light absorption, and photocatalytic
properties of as-prepared samples were studied using various spectroscopic
and analytical techniques. The results showed that Bi<sub>2</sub>O<sub>3</sub>/SiāTiO<sub>2</sub> catalysts held an anatase phase
and possessed high thermal stability. The doped Si was woven into
the lattice of TiO<sub>2</sub>, and its content had a significant
effect on the surface area and the crystal size of Bi<sub>2</sub>O<sub>3</sub>/SiāTiO<sub>2</sub>. The introduced Bi species mainly
existed as oxides on the surface of TiO<sub>2</sub> particles, and
the Bi<sub>2</sub>O<sub>3</sub> photosensitization extended the light
absorption into the visible region. Bi<sub>2</sub>O<sub>3</sub> coupling
also favored the separation and transfer of photoinduced charge carriers
to inhibit their recombination and Si doping enlarged the surface
area of photocatalysts. Compared to bare TiO<sub>2</sub>, Bi<sub>2</sub>O<sub>3</sub>/TiO<sub>2</sub>, and SiāTiO<sub>2</sub>, Bi<sub>2</sub>O<sub>3</sub>/SiāTiO<sub>2</sub> samples showed better
activities for the degradation of methyl orange (MO) and bisphenol
A (BPA) under visible light irradiation (Ī» > 420 nm). The
highest
activity was observed for 1.0% Bi<sub>2</sub>O<sub>3</sub>/15% SiāTiO<sub>2</sub> calcined at 500 Ā°C. The superior performance was ascribed
to the high surface area, the ability to absorb visible light, and
the efficient charge separation associated with the synergetic effects
of appropriate amounts of Si and Bi in the prepared samples. The adsorbed
hydroxyl radicals (<sup>ā¢</sup>OH) were also found to be the
most reactive species in the photocatalytic degradation
Unusual Metallic Microporous Boron Nitride Networks
Two metallic zeolite-like microporous
BN crystals with all-sp<sup>2</sup> bonding networks are predicted
from an unbiased structure
search based on the particle-swarm optimization (PSO) algorithm in
combination with first-principles density functional theory (DFT)
calculations. The stabilities of both microporous structures are confirmed
via the phonon spectrum analysis and BornāOppenheimer molecular
dynamics simulations with temperature control at 1000 K. The unusual
metallicity for the microporous BN allotropes stems from the delocalized
p electrons along the axial direction of the micropores. Both microporous
BN structures entail large surface areas, ranging from 3200 to 3400
m<sup>2</sup>/g. Moreover, the microporous BN structures show a preference
toward organic molecule adsorption (e.g., the computed adsorption
energy for CH<sub>3</sub>CH<sub>2</sub>OH is much more negative than
that of H<sub>2</sub>O). This preferential adsorption can be exploited
for water cleaning, as demonstrated recently using porous boron BN
nanosheets (Nat. Commun. 2013, 4, 1777)
Al<sub><i>x</i></sub>C Monolayer Sheets: Two-Dimensional Networks with Planar Tetracoordinate Carbon and Potential Applications as Donor Materials in Solar Cell
We perform a global search of the
most stable structures of 2D
stoichiometric Al<sub><i>x</i></sub>C (<i>x</i> = 1/3, 1, 2, and 3) monolayer sheets. In the most stable 2D planar
AlC network, every carbon atom is tetracoordinated. In addition to
the structure of AlC, structures of the most stable Al<sub>2</sub>C and Al<sub>3</sub>C monolayer sheets are also predicted for the
first time. AlC and Al<sub>2</sub>C monolayers are semiconducting,
while Al<sub>3</sub>C monolayer is metallic. In particular, Al<sub>2</sub>C monolayer possesses a bandgap of 1.05 eV (based on HSE06
calculation), a value suitable for photovoltaic applications. Moreover,
three Al<sub>2</sub>C/WSe<sub>2</sub>, Al<sub>2</sub>C/MoTe<sub>2</sub>, and AlC/ZnO van der Waals heterobilayers are investigated, and
their power conversion efficiencies are estimated to be in the range
of 12ā18%. The near-perfect match in lattice constants between
the Al<sub>2</sub>C monolayer and PdO (100) surface suggests strong
likelihood of experimental realization of the Al<sub>2</sub>C monolayer
on the PdO (100) substrate
Unusual Metallic Microporous Boron Nitride Networks
Two metallic zeolite-like microporous
BN crystals with all-sp<sup>2</sup> bonding networks are predicted
from an unbiased structure
search based on the particle-swarm optimization (PSO) algorithm in
combination with first-principles density functional theory (DFT)
calculations. The stabilities of both microporous structures are confirmed
via the phonon spectrum analysis and BornāOppenheimer molecular
dynamics simulations with temperature control at 1000 K. The unusual
metallicity for the microporous BN allotropes stems from the delocalized
p electrons along the axial direction of the micropores. Both microporous
BN structures entail large surface areas, ranging from 3200 to 3400
m<sup>2</sup>/g. Moreover, the microporous BN structures show a preference
toward organic molecule adsorption (e.g., the computed adsorption
energy for CH<sub>3</sub>CH<sub>2</sub>OH is much more negative than
that of H<sub>2</sub>O). This preferential adsorption can be exploited
for water cleaning, as demonstrated recently using porous boron BN
nanosheets (Nat. Commun. 2013, 4, 1777)
Unusual Metallic Microporous Boron Nitride Networks
Two metallic zeolite-like microporous
BN crystals with all-sp<sup>2</sup> bonding networks are predicted
from an unbiased structure
search based on the particle-swarm optimization (PSO) algorithm in
combination with first-principles density functional theory (DFT)
calculations. The stabilities of both microporous structures are confirmed
via the phonon spectrum analysis and BornāOppenheimer molecular
dynamics simulations with temperature control at 1000 K. The unusual
metallicity for the microporous BN allotropes stems from the delocalized
p electrons along the axial direction of the micropores. Both microporous
BN structures entail large surface areas, ranging from 3200 to 3400
m<sup>2</sup>/g. Moreover, the microporous BN structures show a preference
toward organic molecule adsorption (e.g., the computed adsorption
energy for CH<sub>3</sub>CH<sub>2</sub>OH is much more negative than
that of H<sub>2</sub>O). This preferential adsorption can be exploited
for water cleaning, as demonstrated recently using porous boron BN
nanosheets (Nat. Commun. 2013, 4, 1777)
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