9 research outputs found
Highly Oxidized Gold Nanoparticles: In Situ Synthesis, Electronic Properties, and Reaction Probability Toward CO Oxidation
Highly oxidized gold nanoparticles
prepared by RF-discharge under
an oxygen atmosphere were studied by X-ray photoelectron spectroscopy
and transmission electron microscopy depending on the particle size.
A surface-like gold oxide was found in the case of small nanoparticles
(1â2 nm) obtained at the first steps of deposition. With an
increase of the particle size up to 5 nm, a bulklike gold oxide was
formed. The O 1s spectra exhibited an oxygen peak at binding energy <i>E</i><sub>b</sub> = 529.4 eV for the surface-like oxide and <i>E</i><sub>b</sub> = 530.7 eV for the bulklike gold-oxide. The
reaction probability of oxidized gold nanoparticles was examined in
the reaction of CO oxidation at room temperature. The surface-like
gold oxide interacted with CO with a high reaction probability of
approximately 0.005, while CO interaction with the bulklike oxide
was characterized by an induction period with lower reaction probability
(0.001). The mechanisms of the interaction of oxidized gold nanoparticles
with CO depending on its size are discussed
XPS Study of Nanostructured Rhodium Oxide Film Comprising Rh<sup>4+</sup> Species
Studies of highly oxidized rhodium
species as potential active
sites in catalytic oxidation reactions are of great interest. In this
work, we investigated the properties of highly oxidized nanostructured
rhodium film prepared by radio frequency discharge in an oxygen atmosphere.
The charge states of Rh in RhO<sub><i>x</i></sub> particles,
their thermal stability, and reactivity toward CO were analyzed in
comparison with the properties of thermally prepared Rh<sub>2</sub>O<sub>3</sub> oxide. The formation of Rh<sup>4+</sup> species in
a composition of Rh<sup>4+</sup>/Rh<sup>3+</sup> oxyhydroxide structures
was shown to take place in plasma-synthesized films. The highly oxidized
rhodium species was stable up to 150 °C and demonstrated reactivity
in a CO oxidation reaction at 100 °C. The reoxidation of a partially
reduced Rh/RhO<sub><i>x</i></sub> film was observed at 100
°C under treatment with molecular O<sub>2</sub>. However, Rh<sup>4+</sup> species were not recovered under such conditions
Stabilization of 1T-MoS<sub>2</sub> Sheets by Imidazolium Molecules in Self-Assembling Hetero-layered Nanocrystals
We report a facile, room-temperature
assembly of MoS<sub>2</sub>-based hetero-layered nanocrystals (NCs)
containing embedded monolayers
of imidazolium (Im), 1-butyl-3-methylÂimidÂazolium (BuMeIm),
2-phenylÂimidÂazolium, and 2-methylÂbenzÂimidÂazolium
molecules. The NCs are readily formed in water solutions by self-organization
of the negatively charged, chemically exfoliated 0.6 nm thick MoS<sub>2</sub> sheets and corresponding cationic imidazole moieties. As
evidenced by transmission electron microscopy, the obtained NCs are
anisotropic in shape, with thickness varying in the range 5â20
nm and lateral dimensions of hundreds of nanometers. The NCs exhibit
almost turbostratic stacking of the MoS<sub>2</sub> sheets, though
the local order is preserved in the orientation of the imidazolium
molecules with respect to the sulfide sheets. The atomic structure
of NCs with BuMeIm molecules was solved from powder X-ray diffraction
data assisted by density functional theory calculations. The performed
studies evidenced that the MoS<sub>2</sub> sheets of the NCs are of
the nonconventional 1T-MoS<sub>2</sub> (metallically conducting) structure.
The sheetsâ puckered outer surface is formed by the S atoms
and the positioning of the BuMeIm molecules follows the sheet nanorelief.
According to thermal analysis data, the presence of the BuMeIm cations
significantly increases the stability of the 1T-MoS<sub>2</sub> modification
and raises the temperature for its transition to the conventional
2H-MoS<sub>2</sub> (semiconductive) counterpart by âŒ70 °C
as compared to pure 1T-MoS<sub>2</sub> (âŒ100 °C). The
stabilizing interaction energy between inorganic and organic layers
was estimated as 21.7 kcal/mol from the calculated electron density
distribution. The results suggest a potential for the design of few-layer
electronic devices exploiting the charge transport properties of monolayer
thin MoS<sub>2</sub>
Stabilization of 1T-MoS<sub>2</sub> Sheets by Imidazolium Molecules in Self-Assembling Hetero-layered Nanocrystals
We report a facile, room-temperature
assembly of MoS<sub>2</sub>-based hetero-layered nanocrystals (NCs)
containing embedded monolayers
of imidazolium (Im), 1-butyl-3-methylÂimidÂazolium (BuMeIm),
2-phenylÂimidÂazolium, and 2-methylÂbenzÂimidÂazolium
molecules. The NCs are readily formed in water solutions by self-organization
of the negatively charged, chemically exfoliated 0.6 nm thick MoS<sub>2</sub> sheets and corresponding cationic imidazole moieties. As
evidenced by transmission electron microscopy, the obtained NCs are
anisotropic in shape, with thickness varying in the range 5â20
nm and lateral dimensions of hundreds of nanometers. The NCs exhibit
almost turbostratic stacking of the MoS<sub>2</sub> sheets, though
the local order is preserved in the orientation of the imidazolium
molecules with respect to the sulfide sheets. The atomic structure
of NCs with BuMeIm molecules was solved from powder X-ray diffraction
data assisted by density functional theory calculations. The performed
studies evidenced that the MoS<sub>2</sub> sheets of the NCs are of
the nonconventional 1T-MoS<sub>2</sub> (metallically conducting) structure.
The sheetsâ puckered outer surface is formed by the S atoms
and the positioning of the BuMeIm molecules follows the sheet nanorelief.
According to thermal analysis data, the presence of the BuMeIm cations
significantly increases the stability of the 1T-MoS<sub>2</sub> modification
and raises the temperature for its transition to the conventional
2H-MoS<sub>2</sub> (semiconductive) counterpart by âŒ70 °C
as compared to pure 1T-MoS<sub>2</sub> (âŒ100 °C). The
stabilizing interaction energy between inorganic and organic layers
was estimated as 21.7 kcal/mol from the calculated electron density
distribution. The results suggest a potential for the design of few-layer
electronic devices exploiting the charge transport properties of monolayer
thin MoS<sub>2</sub>
Electrostatic Origin of Stabilization in MoS<sub>2</sub>âOrganic Nanocrystals
Negatively
charged molybdenum disulfide layers form stable organicâinorganic
layered nanocrystals when reacted with organic cations in solution.
The reasons why this self-assembly process leads to a single-phase
compound with a well-defined interlayer distance in given conditions
are, however, poorly understood to date. Here, for the first time,
we quantify the interactions determining the cation packing and stability
of the MoS<sub>2</sub>âorganic nanocrystals and find that the
main contribution arises from Coulomb forces. The study was performed
on the series of new layered compounds of MoS<sub>2</sub> with naphthalene
derivatives, forming several distinct phases depending on reaction
conditions. Starting with structural models derived from powder X-ray
diffraction data and TEM, we evaluate their cohesion energy by modeling
layer separation with periodic PW-DFT-D calculations. The results
provide a reliable approach for estimation of the stability of MoS<sub>2</sub>-based heterolayered compounds
Electrostatic Origin of Stabilization in MoS<sub>2</sub>âOrganic Nanocrystals
Negatively
charged molybdenum disulfide layers form stable organicâinorganic
layered nanocrystals when reacted with organic cations in solution.
The reasons why this self-assembly process leads to a single-phase
compound with a well-defined interlayer distance in given conditions
are, however, poorly understood to date. Here, for the first time,
we quantify the interactions determining the cation packing and stability
of the MoS<sub>2</sub>âorganic nanocrystals and find that the
main contribution arises from Coulomb forces. The study was performed
on the series of new layered compounds of MoS<sub>2</sub> with naphthalene
derivatives, forming several distinct phases depending on reaction
conditions. Starting with structural models derived from powder X-ray
diffraction data and TEM, we evaluate their cohesion energy by modeling
layer separation with periodic PW-DFT-D calculations. The results
provide a reliable approach for estimation of the stability of MoS<sub>2</sub>-based heterolayered compounds
Different Efficiency of Zn<sup>2+</sup> and ZnO Species for Methane Activation on Zn-Modified Zeolite
Understanding
methane activation pathways on Zn-modified high-silica
zeolites (ZSM-5, BEA) is of particular importance because of the possibility
of methane involvement in coaromatization with higher alkanes on this
type of zeolites. Herein, two samples of Zn-modified zeolite BEA containing
exclusively either small zinc oxide clusters or isolated Zn<sup>2+</sup> cations have been synthesized and thoroughly characterized by a
range of spectroscopic methods (<sup>1</sup>H MAS NMR, DRIFTS, XPS,
EXAFS, HRTEM) to show that only one of the Zn-species, either Zn<sup>2+</sup> cations or ZnO small clusters, exists in the void of zeolite
pores. The ability of zinc sites of different nature to promote the
activation of methane CâH bond with the zeolite BrĂžnsted
acid sites (BAS) has been examined in the reactions of methane H/D
hydrogen exchange with BAS and the alkylation of benzene with methane.
It has been found that both ZnO and Zn<sup>2+</sup> species promote
the reaction of H/D exchange of methane with BAS. The rate of H/D
exchange is higher by 2 and 3 orders of magnitude for the zeolite
loaded with ZnO or Zn<sup>2+</sup> species, respectively, compared
to pure acid-form zeolite H-BEA. So, the promoting effect of Zn<sup>2+</sup> cations is more profound than that of ZnO species for H/D
exchange reaction. This implies that the synergistic effect of Zn-sites
and BAS for CâH bond activation in methane is significantly
higher for Zn<sup>2+</sup> cations compared to small ZnO clusters.
It has been revealed, however, that only Zn<sup>2+</sup> cations promote
the alkylation of benzene with methane, whereas ZnO species do not.
The isolated Zn<sup>2+</sup> cations provide the formation of zinc-methyl
species, which are further transformed to zinc-methoxy species. The
latter is the key intermediate for the performance of the alkylation
reaction. Hence, while both zinc oxide clusters and Zn<sup>2+</sup> cationic species are able to provide a synergistic effect for the
activation of CâH bonds of methane displayed by the dramatic
acceleration of H/D exchange reaction, only the Zn<sup>2+</sup> cationic
species perform methane activation toward the alkylation of benzene
with methane. This implies that only the Zn<sup>2+</sup> cations in
Zn-modified zeolite can activate methane for the reaction of methane
coaromatization with higher alkanes
Bimetallic NiM/C (M = Cu and Mo) Catalysts for the Hydrogen Oxidation Reaction: Deciphering the Role of Unintentional Surface Oxides in the Activity Enhancement
Emerging interest in the platinum group metal (PGM)-free
electrocatalysts
calls for a fundamental understanding of the key factors determining
their activity, the latter being critical for the development of efficient
catalysts. Ni-based materials show high promises as PGM-free anodes
of anion exchange membrane fuel cells (AEMFCs). However, their hydrogen
oxidation reaction (HOR) activity can differ by several orders of
magnitude, and the factors responsible for this are still being debated.
In this work, the effect of unintentional surface oxides in Ni/C and
NiM/C (M = Cu and Mo) is revealed by benchmarking either the catalysts
conventionally stored under ambient conditions or purposely reduced
âoxide-freeâ materials. The analysis of electrocatalytic
data complemented by detailed material characterization, Monte Carlo
simulations, and density functional calculations, underlines the key
importance of surface oxides in the HOR catalysis on Ni, NiCu, and
NiMo electrodes. These findings underscore the need to measure the
HOR activity of Ni-based catalysts in the absence of surface oxides
in order to unambiguously interpret the influence of other factors
(such as the electronic effect of the second element) on activity
enhancement
Platinum Acetate Blue: Synthesis and Characterization
Platinum
acetate blue (PAB) of the empirical formula PtÂ(OOCMe)<sub>2.5±0.25</sub>, a byproduct in the synthesis of crystalline platinumÂ(II) acetate
Pt<sub>4</sub>(OOCMe)<sub>8</sub>, is an X-ray amorphous substance
containing platinum in the oxidation state between (II) and (III).
Typical PAB samples were studied with X-ray diffraction, differential
thermal analysisâthermogravimetric, extended X-ray absorption
fine structure, scanning electron microscopy, transmission electron
microscopy, magnetochemistry, and combined quantum chemical density
functional theoryâmolecular mechanics modeling to reveal the
main structural features of the PAB molecular building blocks. The
applicability of PAB to the synthesis of platinum complexes was demonstrated
by the preparation of the new homo- and heteronuclear complexes Pt<sup>II</sup>(dipy)Â(OOCMe)<sub>2</sub> (<b>1</b>), Pt<sup>II</sup>(ÎŒ-OOCMe)<sub>4</sub>Co<sup>II</sup>(OH<sub>2</sub>) (<b>2</b>), and Pt<sup>III</sup><sub>2</sub>(OOCMe)<sub>4</sub>(O<sub>3</sub>SPhMe)<sub>2</sub> (<b>3</b>) with the use of PAB as
starting material