47 research outputs found
Monoethanolamine Adsorption on TiO<sub>2</sub>(110): Bonding, Structure, and Implications for Use as a Model Solid-Supported CO<sub>2</sub> Capture Material
We have studied the adsorption of
monoethanolamine (MEA, HO(CH<sub>2</sub>)<sub>2</sub>NH<sub>2</sub>), a well-known CO<sub>2</sub> capture
molecule, on the rutile TiO<sub>2</sub>(110) surface using a combined
experimental and theoretical approach. X-ray photoelectron spectroscopy,
near-edge X-ray absorption fine structure spectroscopy, and scanning
tunneling microscopy measurements indicate that MEA adsorbs with the
oxygen atom of the hydroxyl group and the nitrogen atom of the amine
group bonded to adjacent 5-fold coordinated Ti-sites (Ti(5f)) in the
Ti-troughs, leading to a saturation coverage of 0.5 ML at room temperature.
Density functional theory calculations confirm that this adsorption
configuration is the most stable one with an adsorption energy of
2.33 eV per MEA molecule. The bonding of MEA to TiO<sub>2</sub>(110)
is dominated by local donor–acceptor bonds between the oxygen
and nitrogen atoms of the MEA molecule and surface Ti(5f) sites. Hydrogen
bonds between adjacent MEA molecules stabilize the adsorption structure
at saturation coverage. The implications of this bonding configuration
for the use of MEA/TiO<sub>2</sub>(110) as a model CO<sub>2</sub> capture
material will be discussed
Tuning Selectivity in the Direct Conversion of Methane to Methanol: Bimetallic Synergistic Effects on the Cleavage of C–H and O–H Bonds over NiCu/CeO<sub>2</sub> Catalysts
The efficient activation
of methane and the simultaneous water
dissociation are crucial in many catalytic reactions on oxide-supported
transition metal catalysts. On very low-loaded Ni/CeO2 surfaces,
methane easily fully decomposes, CH4 → C + 4H, and
water dissociates, H2O→ OH + H. However, in important
reactions such as the direct oxidation of methane to methanol (MTM),
where complex interplay exists between reactants (CH4,
O2), it is desirable to avoid the complete dehydrogenation
of methane to carbon. Remarkably, the barrier for the activation of
C–H bonds in CHx (x = 1–3) species on Ni/CeO2 surfaces can be manipulated
by adding Cu, forming bimetallic NiCu clusters, whereas the ease for
cleavage of O–H bonds in water is not affected by ensemble
effects, as obtained from density functional theory-based calculations.
CH4 activation occurs only on Ni sites, and H2O activation occurs on both Ni and Cu sites. The MTM reaction pathway
for the example of the Ni3Cu1/CeO2 model catalyst predicts a higher selectivity and a lower activation
barrier for methanol production, compared with that for Ni4/CeO2. These findings point toward a possible strategy
to design active and stable catalysts which can be employed for methane
activation and conversions
<i>In Situ</i> Formation of FeRh Nanoalloys for Oxygenate Synthesis
Early
and late transition metals are often combined as a strategy
to tune the selectivity of catalysts for the conversion of syngas
(CO/H<sub>2</sub>) to C<sub>2+</sub> oxygenates, such as ethanol.
Here we show how the use of a highly reducible Fe<sub>2</sub>O<sub>3</sub> support for Rh leads to the <i>in situ</i> formation
of supported FeRh nanoalloy catalysts that exhibit high selectivity
for ethanol synthesis. <i>In situ</i> characterizations
by X-ray diffraction (XRD) and X-ray absorption spectroscopy (XAS)
reveal the coexistence of iron oxide, iron carbide, metallic iron,
and FeRh alloy phases depending on reaction conditions and Rh loading.
Structural analysis coupled with catalytic testing indicates that
oxygenate formation is correlated to the presence of FeRh alloys,
while the iron oxide and carbide phases lead mainly to hydrocarbons.
The formation of nanoalloys by <i>in situ</i> reduction
of a metal oxide support under working conditions represents a simple
approach for the preparation bimetallic catalysts with enhanced catalytic
properties
Enhanced Stability of Pt-Cu Single-Atom Alloy Catalysts: In Situ Characterization of the Pt/Cu(111) Surface in an Ambient Pressure of CO
The interaction between a catalyst
and reactants often induces
changes in the surface structure and composition of the catalyst,
which, in turn, affect its reactivity. Therefore, it is important
to study such changes using in situ techniques under well-controlled
conditions. We have used ambient pressure X-ray photoelectron spectroscopy
to study the surface stability of a Pt/Cu(111) single-atom alloy in
an ambient pressure of CO. By directly probing the Pt atoms, we found
that CO causes a slight surface segregation of Pt atoms at room temperature.
In addition, while the Pt/Cu(111) surface demonstrates poor thermal
stability in ultrahigh vacuum conditions, where surface Pt starts
to diffuse to the subsurface layer above 400 K, the presence of adsorbed
CO enhances the thermal stability of surface Pt atoms. However, we
also found that temperatures above 450 K cause restructuring of the
subsurface layer, which consequently strengthens the CO binding to
the surface Pt sites, likely because of the presence of neighboring
subsurface Pt atoms
Low-Temperature Conversion of Methane to Methanol on CeO<sub><i>x</i></sub>/Cu<sub>2</sub>O Catalysts: Water Controlled Activation of the C–H Bond
An inverse CeO<sub>2</sub>/Cu<sub>2</sub>O/Cu(111) catalyst is
able to activate methane at room temperature producing C, CH<sub><i>x</i></sub> fragments and CO<sub><i>x</i></sub> species
on the oxide surface. The addition of water to the system leads to
a drastic change in the selectivity of methane activation yielding
only adsorbed CH<sub><i>x</i></sub> fragments. At a temperature
of 450 K, in the presence of water, a CH<sub>4</sub> → CH<sub>3</sub>OH catalytic transformation occurs with a high selectivity.
OH groups formed by the dissociation of water saturate the catalyst
surface, removing sites that could decompose CH<sub><i>x</i></sub> fragments, and generating centers on which methane can directly
interact to yield methanol
Understanding the Surface Structure and Catalytic Activity of SnO<sub><i>x</i></sub>/Au(111) Inverse Catalysts for CO<sub>2</sub> and H<sub>2</sub> Activation
Carbon
dioxide hydrogenation is a promising approach for the reduction
of greenhouse gas pollution via the production of fuels and high-value
chemicals utilizing C1 chemistry. In this process, the activation
of nonpolar molecules, CO2 and H2, at mild conditions
is challenging. Herein, we report a well-defined inverse SnOx/Au(111) catalyst that shows the ability to activate
both CO2 and H2 at room temperature. Scanning
tunneling microscopy (STM) and ambient pressure X-ray photoemission
spectroscopy (AP-XPS) are combined to understand the surface structure,
growth mode, chemical state, and activity of SnOx/Au(111) surfaces. Nanostructures of SnOx at the sub-monolayer level were prepared by depositing Sn
on Au(111) followed by O2 oxidation. For the as-prepared
SnOx/Au(111), two-dimensionally formed
SnOx thin films on a Au(111) substrate
were observed with STM of two different moieties, discernible based
on their height: clusters (∼0.4 Å) and nanoparticles (NPs,
1–2.5 Å), which are assigned to Sn–Au alloys and
SnOx, respectively, in corroboration with
XPS analysis. Furthermore, SnOx/Au(111)
was annealed under UHV to test its thermal stability. Upon annealing
at 400–600 K, a disappearance of SnOx NPs and reappearance of highly dispersed Sn clusters were
clearly noticeable from the STM and XPS results, identifying the thermal
decomposition of SnOx and subsequent formation
of Sn–Au alloys on the surface due to the recombination of
Sn clusters with Au. We investigated the reactivity of the SnOx/Au(111) surfaces toward CH4,
CO2, and H2. The SnOx/Au(111) surfaces have excellent CO2 and H2 activation abilities even at room temperature with negligible reactivity
for methane activation. Our AP-XPS results show that H2 can be activated on the SnOx NPs by
the reduction to Sn. For CO2, the activation and further
dissociation are identified by a reoxidation of Sn with newly formed
Sn–O bonds and the formation of surface carbon. Therefore,
we propose that SnOx is a potential catalyst
or additive to achieve CO2 hydrogenation under mild conditions
Effect of Chloride Anions on the Synthesis and Enhanced Catalytic Activity of Silver Nanocoral Electrodes for CO<sub>2</sub> Electroreduction
Metallic silver (Ag) is known as
an efficient electrocatalyst for
the conversion of carbon dioxide (CO<sub>2</sub>) to carbon monoxide
(CO) in aqueous or nonaqueous electrolytes. However, polycrystalline
silver electrocatalysts require significant overpotentials in order
to achieve high selectivity toward CO<sub>2</sub> reduction, as compared
to the side reaction of hydrogen evolution. Here we report a high-surface-area
Ag nanocoral catalyst, fabricated by an oxidation–reduction
method in the presence of chloride anions in an aqueous medium, for
the electro-reduction of CO<sub>2</sub> to CO with a current efficiency
of 95% at the low overpotential of 0.37 V and the current density
of 2 mA cm<sup>–2</sup>. A lower limit of TOF of 0.4 s<sup>–1</sup> and TON > 8.8 × 10<sup>4</sup> (over 72 h)
was
estimated for the Ag nanocoral catalyst at an overpotential of 0.49
V. The Ag nanocoral catalyst demonstrated a 32-fold enhancement in
surface-area-normalized activity, at an overpotential of 0.49 V, as
compared to Ag foil. We found that, in addition to the effect on nanomorphology,
the adsorbed chloride anions play a critical role in the observed
enhanced activity and selectivity of the Ag nanocoral electrocatalyst
toward CO<sub>2</sub> reduction. Synchrotron X-ray photoelectron spectroscopy
(XPS) studies along with a series of control experiments suggest that
the chloride anions, remaining adsorbed on the catalyst surface under
electrocatalytic conditions, can effectively inhibit the side reaction
of hydrogen evolution and enhance the catalytic performance for CO<sub>2</sub> reduction
Reduction of Nano-Cu<sub>2</sub>O: Crystallite Size Dependent and the Effect of Nano-Ceria Support
Copper(I) oxide (Cu<sub>2</sub>O)
is an effective catalyst in the
CO oxidation reaction. While high surface to volume ratio in nanoparticles
will increase their catalytic efficiency, it posts a stability problem.
Here we study the stability of nano-cuprite against reduction as a
function of its crystallite size and upon interaction with a nano-ceria
support. A systematic analysis of isothermal reduction of a series
size of monodispersed Cu<sub>2</sub>O nanocrystals (±7%) with
time-resolved X-ray diffraction (TR-XRD) provides the time-resolved
phase fraction of Cu<sub>2</sub>O and the time when reduction product
of Cu (fcc) first appears. The initial phase fraction of nano-Cu<sub>2</sub>O is less than one with the balance attributed to an amorphous
CuO shell. Since no peaks of crystalline CuO (monoclinic) were observed,
a core–shell structure with an amorphous CuO shell is proposed.
From the analysis, Cu<sup>2+</sup> content in corresponding to shell
increases from 0 to 33% as Cu<sub>2</sub>O decreases to 8 nm from
the bulk. Based on the reduction profiles, a time size reduction (TSR)
diagram is constructed for the observed Cu<sub>2</sub>O phase behavior
during reduction. The incorporation onto a nano-CeO<sub>2</sub> support
(7 nm) significantly stabilizes our nano-Cu<sub>2</sub>O in a reducing
atmosphere. The oxygen supply propensity in terms of oxygen nonstoichiometry
of CeO<sub>2–<i>y</i></sub> is shown to be lower
when a larger crystallite size CeO<sub>2</sub> (20 nm) support is
used. The larger oxygen capacity in smaller nano-CeO<sub>2</sub> support
is analyzed and explained by the “Madelung model” with
size-dependent bulk modulus of nano-ceria
Tuning the Placement of Pt “Single Atoms” on a Mixed CeO<sub>2</sub>–TiO<sub>2</sub> Support
Defect
sites on the oxide supports can be used to anchor and activate
“single-atom” catalysts (SACs). By engineering the anchoring
sites for supporting SACs, one can alter their electronic and atomic
structures which, in turn, define their activity, selectivity, and
stability for catalytic reactions. To create and tune unique sites
for Pt SACs on CeO2 support, in this work, we synthesized
a system consisting of CeO2 decorated on TiO2 nano-oxides for supporting the Pt SACs and investigated the effect
of Pt weight loading. A combination of multiple structural characterization
methods including diffuse reflectance infrared Fourier transform spectroscopy
(DRIFTS), X-ray photoelectron spectroscopy (XPS), and X-ray absorption
spectroscopy (XAS) was employed to characterize the distribution of
charge states of single atoms and evaluate the heterogeneity of their
binding sites. We have found that the placement of Pt atoms can be
tuned on a mixed oxide surface by changing the weight loading of Pt
Implementation of New TPD Analysis Techniques in the Evaluation of Second Order Desorption Kinetics of Cyanogen from Cu(001)
The interactions of cyanide species with a copper (001) surface were studied with temperature programmed desorption (TPD) and X-ray photoelectron spectroscopy (XPS). Adsorbed cyanide species (CN(a)) undergo recombinative desorption evolving molecular cyanogen (C2N2). As the adsorbed CN species charge upon adsorption, mutually repulsive dipolar interactions lead to a marked desorption energy reduction with increasing CN(a) coverages. Two new TPD analysis approaches were developed, which used only accurately discernible observables and which do not assume constant desorption energies, Ed, and pre-exponential values, ν. These two approaches demonstrated a linear variation of Ed with instantaneous coverage. The first approach involved an analysis of the variations of desorption peak asymmetry with initial CN coverages. The second quantitative approach utilized only temperatures and intensities of TPD peaks, together with deduced surface coverages at the peak maxima, also as a function of initial surface coverages. Parameters derived from the latter approach were utilized as initial inputs for a comprehensive curve fit analysis technique. Excellent fits for all experimental desorption curves were produced in simulations. The curve fit analysis confirms that the activation energy of desorption of 170−180 kJ/mol at low coverage decreases by up to 14−15 kJ/mol at CN saturation
