6 research outputs found
Effect of Passivation on Stability and Electronic Structure of Bulk-like ZnO Clusters
Electronic structure
of nearly stoichiometric and nonstoichiometric
clusters of ZnO having bulk-like wurtzite geometry passivated with
fictitious hydrogen atoms are comparatively analyzed for structural
evolution using density functional theory-based electronic structure
calculations. A parameter, average binding energy per atomic number
(ABE-number), is introduced for better insight of structural evolution.
The stability of a cluster is determined by binding energy per atom
and ABE-number, whereas structural evolution on the basis of spin-polarized
energy spectrum is studied via site projected partial density of states
(l-DOS). The overall structural evolution is mapped for bare and passivated
ZnO clusters to l-DOS. The study has established a correlation between
the stability of clusters and their l-DOS. O-excess and O-surfaced
clusters are found to be more stable. The HOMO–LUMO gap varies
from 0 to 6.3 eV by tuning the size, composition, and surface termination
of the clusters. Present results reported for clusters of sizes up
to ∼1 nm can pave a path for formulating strategies for experimental
synthesis of ZnO nanoparticles for tuning the HOMO–LUMO gap
Ethylenediamine-Mediated Wurtzite Phase Formation in ZnS
The usual high temperature wurtzite
phase of ZnS was successfully
obtained at low temperature (170 °C) in the presence of ethylenediamine
(EN) as the soft template. X-ray diffraction and Raman spectroscopy
analysis confirmed the EN-mediated phase transformation (zinc blende
to wurtzite) of ZnS. X-ray photoelectron spectroscopy (XPS) showed
that all the samples were sulfur deficient. A high temperature X-ray
diffraction (XRD) study showed that ZnS samples, both EN-mediated
and without EN, retained their phases except small changes in the
unit cell dimension. Besides the EN-mediated phase transition, morphology
transformations from nearly spherical shape to nanorods are also observed
by scanning electron microscopy (SEM) and transmission electron microscopy
(TEM). The coupling between EN molecules with ZnS is confirmed by
Fourier transform infrared spectroscopy. A significant reduction in
the phase transition temperature of ZnS has been achieved as compared
to the bulk transition temperature (1020 °C). Mechanisms of phase
transformation have been discussed. The density functional theory
(DFT) supports the rod formation and wurtzite structure in the presence
of nitrogen-terminated ZnS surface
Ethylenediamine-Mediated Wurtzite Phase Formation in ZnS
The usual high temperature wurtzite
phase of ZnS was successfully
obtained at low temperature (170 °C) in the presence of ethylenediamine
(EN) as the soft template. X-ray diffraction and Raman spectroscopy
analysis confirmed the EN-mediated phase transformation (zinc blende
to wurtzite) of ZnS. X-ray photoelectron spectroscopy (XPS) showed
that all the samples were sulfur deficient. A high temperature X-ray
diffraction (XRD) study showed that ZnS samples, both EN-mediated
and without EN, retained their phases except small changes in the
unit cell dimension. Besides the EN-mediated phase transition, morphology
transformations from nearly spherical shape to nanorods are also observed
by scanning electron microscopy (SEM) and transmission electron microscopy
(TEM). The coupling between EN molecules with ZnS is confirmed by
Fourier transform infrared spectroscopy. A significant reduction in
the phase transition temperature of ZnS has been achieved as compared
to the bulk transition temperature (1020 °C). Mechanisms of phase
transformation have been discussed. The density functional theory
(DFT) supports the rod formation and wurtzite structure in the presence
of nitrogen-terminated ZnS surface
Ethylenediamine-Mediated Wurtzite Phase Formation in ZnS
The usual high temperature wurtzite
phase of ZnS was successfully
obtained at low temperature (170 °C) in the presence of ethylenediamine
(EN) as the soft template. X-ray diffraction and Raman spectroscopy
analysis confirmed the EN-mediated phase transformation (zinc blende
to wurtzite) of ZnS. X-ray photoelectron spectroscopy (XPS) showed
that all the samples were sulfur deficient. A high temperature X-ray
diffraction (XRD) study showed that ZnS samples, both EN-mediated
and without EN, retained their phases except small changes in the
unit cell dimension. Besides the EN-mediated phase transition, morphology
transformations from nearly spherical shape to nanorods are also observed
by scanning electron microscopy (SEM) and transmission electron microscopy
(TEM). The coupling between EN molecules with ZnS is confirmed by
Fourier transform infrared spectroscopy. A significant reduction in
the phase transition temperature of ZnS has been achieved as compared
to the bulk transition temperature (1020 °C). Mechanisms of phase
transformation have been discussed. The density functional theory
(DFT) supports the rod formation and wurtzite structure in the presence
of nitrogen-terminated ZnS surface
Band Gap Bowing at Nanoscale: Investigation of CdS<sub><i>x</i></sub>Se<sub>1–<i>x</i></sub> Alloy Quantum Dots through Cyclic Voltammetry and Density Functional Theory
The band gap bowing effect in oleic
acid-stabilized CdS<sub><i>x</i></sub>Se<sub>1–<i>x</i></sub> alloy quantum
dots (Q-dots) with varying composition has been studied experimentally
by means of cyclic voltammetry and theoretically using density functional
theory based calculations. Distinct cathodic and anodic peaks observed
in the cyclic voltammograms of diffusing quantum dots alloy are attributed
to the respective conduction and valence band edges. The quasi-particle
gap values determined from voltammetric measurements are compared
with interband transition peaks in UV–vis and PL spectra. Electronic
structure for alloy Q-dots is determined computationally with projector
augmented wave method for a particular size of dots. The band gap
bowing is observed predominantly in the conduction band states. The
bowing parameter determined experimentally (0.45 eV) has been found
to be in good agreement with the one estimated from DFT (0.43 eV)
Electronic Structure of Visible Light-Driven Photocatalyst δ‑Bi<sub>11</sub>VO<sub>19</sub> Nanoparticles Synthesized by Thermal Plasma
Size confinement for tailoring of
electronic structures can in
principle be explored for enhancement of photocatalytic properties.
In the present work, vanadium-doped bismuth oxide nanoparticles, with
an average particle size of 36 nm, are synthesized for the first time,
using the thermal plasma method, in large scale with high yield to
explore for photocatalytic applications. The electronic and crystallographic
structures of the sample are studied experimentally and theoretically.
Systematic investigations of the electronic structure of the fluorite
type cubic phase of Bi<sub>11</sub>VO<sub>19</sub> nanoparticles are
reported for the first time. Enhancement is observed in the photocatalytic
activity as compared to other delta phases of bismuth vanadate. The
valence band is found to comprise mainly of O 2p states, whereas the
conduction band arises from V 3d states giving rise to a band gap
value of 2.26 eV. Absence of excess O in δ-Bi<sub>2</sub>O<sub>3</sub> results in shrinking of the band gap because of O 2p, Bi
6s and 6p states from the surrounding atoms at doping sites. Bi<sub>11</sub>VO<sub>19</sub> nanoparticles show an efficient visible light
absorption and exhibit excellent photodegradation properties of methylene
blue solution under visible light irradiation