8 research outputs found
Amino Acid Analogue-Conjugated BN Nanomaterials in a Solvated Phase: First Principles Study of Topology-Dependent Interactions with a Monolayer and a (5,0) Nanotube
Using density functional theory and
an implicit solvation model,
the relationship between the topology of boron nitride (BN) nanomaterials
and the protonated/deprotonated states of amino acid analogues is
investigated. In the solvated phase, the calculated results show distinct
āphysisorbed versus chemisorbedā conditions for the
analogues of arginine (Arg)- and aspartic acid (Asp)-conjugated BN
nanomaterials, including a monolayer (ML) and a small-diameter zigzag
nanotube (NT). Such a distinction does not depend on the functional
groups of amino acids but rather depends on the curvature-induced
interactions associated with the tubular configuration. Arg and Asp
interact with the BNML to form physisorbed complexes irrespective
of the state of the amino acids in the solvated phase. For the NT,
Arg and Asp form chemisorbed complexes, and the distinct nature of
bonds between the donor electron moieties of N<sub>(Arg)</sub> and
O<sub>(Asp)</sub> and the boron of the tubular surface is revealed
by the natural bond orbital analysis; stronger s-type bonds for the
deprotonated conjugated complexes and slightly weaker p-type dominated
bonds for the protonated conjugated complexes. The interaction of
neutral Trp with BN nanomaterials results in physisorbed configurations
through Ļ-stacking interactions with the indole ring of the
Trp and BN nanomaterials. The calculated results form the basis for
a theoretical study of more complex protein macromolecules interacting
with nanomaterials under physiological conditions
Controlling the Performance of a Three-Terminal Molecular Transistor: Conformational versus Conventional Gating
The effect of conformational changes in the gate arm
of a three-terminal
device is investigated. In the ground state, the gate (triphenyl)
arm is nonplanar, where the middle phenyl ring is approximately 30Ā°
out-of-plane relative to other two rings. At this geometry, the calculated
tunnel current (<i>I</i><sub>d</sub>) as a function of external
bias (<i>V</i><sub>ds</sub>) across the two DāA substituted
arms exhibits a typical insulator-semiconductor behavior. Similar <i>I</i><sub>d</sub>ā<i>V</i><sub>ds</sub> characteristics
is calculated when planarity of the triphenyl arm is restored. However,
a significant increase, by more than an order of magnitude, and a
distinct variation in the current are predicted in its operational
mode (<i>V</i><sub>ds</sub> > 1.5 V) when additional
nonplanarity
is induced in the triphenyl chain. Analysis of the results suggest
that, unlike in āvoltageā gating, neither the HOMOāLUMO
gap nor the dipole moment of the system undergo significant changes
due to pure conformational gating, as observed in this study. Instead,
the observed conformational gating affects the current via localization/delocalization
of the electronic wave function in the conduction channel. Furthermore,
the tunneling current corresponding to conformational gating in two
different directions appears to exhibit oscillatory nature with a
phase factor of Ļ/2 in the presence of the gate field. The current
modulation is found to reach its maximum only under exclusive effect
of voltage or conformational gating and diminishes when both of them
are present
Hierarchical Self-Assembly of Noncanonical Guanine Nucleobases on Graphene
Self-assembly characterizes the fundamental
basis toward realizing
the formation of highly ordered hierarchical heterostructures. A systematic
approach toward the supramolecular self-assembly of free-standing
guanine nucleobases and the role of graphene as a substrate in directing
the monolayer assembly are investigated using the molecular dynamics
simulation. We find that the free-standing bases in gas phase aggregate
into clusters dominated by intermolecular H-bonds, whereas in solvent,
substantial screening of intermolecular interactions results in Ļ-stacked
configurations. Interestingly, graphene facilitates the monolayer
assembly of the bases mediated through the baseāsubstrate ĻāĻ
stacking. The bases assemble in a highly compact network in gas phase,
whereas in solvent, a high degree of immobilization is attributed
to the disruption of intermolecular interactions. Graphene-induced
stabilization/aggregation of free-standing guanine bases appears as
one of the prerequisites governing molecular ordering and assembly
at the solid/liquid interface. The results demonstrate an interplay
between intermolecular and Ļ-stacking interactions, central
to the molecular recognition, aggregation dynamics, and patterned
growth of functional molecules on two-dimensional nanomaterials
Can Single-Atom Change Affect Electron Transport Properties of Molecular Nanostructures such as C<sub>60</sub> Fullerene?
At the nanoscale, even a single atom change in the structure can noticeably alter the properties, and therefore, the application space of materials. We examine this critical behavior of nanomaterials using fullerene as a model structure by a first-principles density functional theory method coupled with nonequilibrium Greenās function formalism. Two different configurations, namely, (i) endohedral (B@C<sub>60</sub> and N@C<sub>60</sub>), in which the doping atom is encapsulated inside the fullerene cage, and (ii) substitutional (BC<sub>59</sub> and NC<sub>59</sub>), in which the doping atom replaces a C atom on the fullerene cage, are considered. The calculated results reveal that the conductivity for the doped fullerene is higher than that of the pristine fullerene. In the low-bias regime, the current (I) voltage (V) characteristic of the endohedral as well as the substitutional configurations are very similar. However, as the external bias increases beyond 1.0 V, the substitutional BC<sub>59</sub> fullerene exhibits a considerably higher magnitude of current than all other species considered, thus suggesting that it can be an effective semiconductor in <i>p</i>-type devices
Nature of Interaction between Semiconducting Nanostructures and Biomolecules: Chalcogenide QDs and BNNT with DNA Molecules
Interactions of DNA oligomers with
two categories of semiconducting
nanostructuresīøchalcogenide quantum dots (QDs) and boron nitride
nanotubes (BNNTs)īøowing to their widespread presence in bio-inspired
processes are investigated using the first-principles density functional
theory and continuum solvent model. The chalcogenide QDs interact
strongly at their metal centers featuring electrostatic interaction
with DNA oligomers at oxygen or nitrogen site, while BNNTs form covalent
bonds with DNA oligomers at multiple surface sites. It is found that
the different bonding nature leads to distinctly different response
to the aqueous environment; the presence of solvent drastically reduces
the binding strength of nucleobases with the QDs due to the strong
electrostatic screening. This is not the case with BNNTs for which
the covalent bonding is barely affected by the solvent. This study
thus clearly shows how a solvent medium influences chemical interactions
providing guidance for technological applications of bioconjugated
systems
Real-Time Electrochemical Monitoring of Adenosine Triphosphate in the Picomolar to Micromolar Range Using Graphene-Modified Electrodes
We
report on a competitive electrochemical detection system that
is free of wash steps and enables the real-time monitoring of adenosine
triphosphate (ATP) in a quantitative manner over a five-log concentration
range. The system utilizes a recognition surface based on ATP aptamer
(ATPA) capture probes prebound to electroactive flavin adenine dinucleotide
(FAD) molecules, and a signaling surface utilizing graphene (Gr) and
gold nanoparticle (AuNP) modified carbon paste electrode (GrāAuNPāCPE)
that is optimized to enhance electron-transfer kinetics and signal
sensitivity. Binding of ATP to ATPA at the recognition surface causes
the release of an equivalent concentration of FAD that can be quantitatively
monitored in real time at the signaling surface, thereby enabling
a wide linear working range (1.14 Ć 10<sup>ā10</sup> to
3.0 Ć 10<sup>ā5</sup> M), a low detection limit (2.01
Ć 10<sup>ā11</sup> M using graphene and AuNP modified
glassy carbon), and fast target binding kinetics (steady-state signal
within 12 min at detection limit). Unlike assays based on capture
probe-immobilized electrodes, this double-surface competitive assay
offers the ability to speed up target binding kinetics by increasing
the capture probe concentration, with no limitations due to intermolecular
Coulombic interactions and nonspecific binding. We utilize the real-time
monitoring capability to compute kinetic parameters for target binding
and to make quantitative distinctions on degree of base-pair mismatch
through monitoring target binding kinetics over a wide concentration
range. On the basis of the simplicity of the assay chemistry and the
quantitative detection of ATP within fruit and serum media, as demonstrated
by comparison of ATP levels against those determined using a standard
high-performance liquid chromatography (HPLC)-UV absorbance method,
we envision a versatile detection platform for applications requiring
real-time monitoring over a wide target concentration range
<i>In situ</i> Synthesis of Fluorescent Gold Nanoclusters by Nontumorigenic Microglial Cells
To date, the directed <i>in
situ</i> synthesis of fluorescent
gold nanoclusters (AuNCs) has only been demonstrated in cancerous
cells, with the theorized synthesis mechanism prohibiting AuNC formation
in nontumorigenic cell lines. This limitation hinders potential biostabilized
AuNC-based technology in healthy cells involving both chemical and
mechanical analysis, such as the direct sensing of protein function
and the elucidation of local mechanical environments. Thus, new synthesis
strategies are required to expand the application space of AuNCs beyond
cancer-focused cellular studies. In this contribution, we have developed
the methodology and demonstrated the direct <i>in situ</i> synthesis of AuNCs in the nontumorigenic neuronal microglial line,
C8B4. The as-synthesized AuNCs form <i>in situ</i> and are
stabilized by cellular proteins. The clusters exhibit bright green
fluorescence and demonstrate low (<10%) toxicity. Interestingly,
elevated ROS levels were not required for the <i>in situ</i> formation of AuNCs, although intracellular reductants such as glutamate
were required for the synthesis of AuNCs in C8B4 cells. To our knowledge,
this is the first-ever demonstration of AuNC synthesis in nontumorigenic
cells and, as such, it considerably expands the application space
of biostabilized fluorescent AuNCs
Growth of Large Single-Crystalline Two-Dimensional Boron Nitride Hexagons on Electropolished Copper
Hexagonal-boron
nitride (h-BN) or āwhite grapheneā
has many outstanding properties including high thermal conductivity,
high mechanical strength, chemical inertness, and high electrical
resistance, which open up a wide range of applications such as thermal
interface material, protective coatings, and dielectric in nanoelectronics
that easily exceed the current advertised benefits pertaining to the
graphene-based applications. The development of h-BN films using chemical
vapor deposition (CVD) has thus far led into nucleation of triangular
or asymmetric diamond shapes on different metallic surfaces. Additionally,
the average size of the triangular domains has remained relatively
small (ā¼0.5 Ī¼m<sup>2</sup>) leading to a large number
of grain boundaries and defects. While the morphology of Cu surfaces
for CVD-grown graphene may have impacts on the nucleation density,
domain sizes, thickness, and uniformity, the effects of the decreased
roughness of Cu surface to develop h-BN films are unknown. Here, we
report the growth and characterization of novel large area h-BN hexagons
using highly electropolished Cu substrate under atmospheric pressure
CVD conditions. We found that the nucleation density of h-BN is significantly
reduced while domain sizes increase. In this study, the largest hexagonal-shape
h-BN domain observed is 35 Ī¼m<sup>2</sup>, which is an order
of magnitude larger than a typical triangular domain. As the domains
coalesce to form a continuous film, the larger grain size offers a
more pristine and smoother film with lesser grain boundaries induced
defects