29 research outputs found
EMSL and Institute for Integrated Catalysis (IIC) Catalysis Workshop
Within the context of significantly accelerating scientific progress in research areas that address important societal problems, a workshop was held in November 2010 at EMSL to identify specific and topically important areas of research and capability needs in catalysis-related science
Origin of Coverage Dependence in Photoreactivity of Carboxylate on TiO<sub>2</sub>(110): Hindering by Charged Coadsorbed Hydroxyls
The influence of reactant coverage
on photochemical activity was
explored using scanning tunneling microscopy (STM) and ultraviolet
photoelectron spectroscopy (UPS). We observed diminished reactivity
of carboxylate species (trimethyl acetate, TMA) on TiO<sub>2</sub>(110) as a function of increasing coverage. This effect was not linked
to intermolecular interactions of TMA but to the accumulation of the
coadsorbed bridging hydroxyls (HO<sub>b</sub>) deposited during (thermal)
dissociative adsorption of the parent, trimethylacetic acid (TMAA).
Confirmation of the hindering influence of HO<sub>b</sub> groups was
obtained by the observation that HO<sub>b</sub> species originated
from H<sub>2</sub>O dissociation at O-vacancy sites have a similar
hindering effect on TMA photochemistry. Though HO<sub>b</sub>’s
are photoinactive on TiO<sub>2</sub>(110) under ultrahigh vacuum conditions,
UPS results show that these sites trap photoexcited electrons, which
in turn likely (electrostatically) attract and neutralize photoexcited
holes, thus suppressing the hole-mediated photoreactivity of TMA.
This negative influence of surface hydroxyls on hole-mediated photochemistry
is likely a major factor in other anaerobic photochemical processes
on reducible oxide surfaces
Direct Observation of Site-Specific Molecular Chemisorption of O<sub>2</sub> on TiO<sub>2</sub>(110)
Molecularly chemisorbed O<sub>2</sub> species were directly imaged on reduced TiO<sub>2</sub>(110) at 50 K with high-resolution scanning tunneling microscopy (STM). Two different O<sub>2</sub> adsorption channels, one at bridging oxygen vacancies (V<sub>O</sub>) and another at 5-fold coordinated terminal titanium atoms (Ti<sub>5c</sub>), have been identified. While O<sub>2</sub> species at the Ti<sub>5c</sub> site appears as a single protrusion centered on the Ti<sub>5c</sub> row, the O<sub>2</sub> at V<sub>O</sub> manifests itself by a disappearance of the V<sub>O</sub> feature. It is found that the STM tip can easily dissociate O<sub>2</sub> species, unless extremely low magnitude of the tunneling parameters are used. The O<sub>2</sub> molecules chemisorbed at low temperatures at these two distinct sites are the most likely precursors for the two O<sub>2</sub> dissociation channels, observed at temperatures above 150 and 230 K at the V<sub>O</sub> and Ti<sub>5c</sub> sites, respectively
Characterization of the Active Surface Species Responsible for UV-Induced Desorption of O<sub>2</sub> from the Rutile TiO<sub>2</sub>(110) Surface
We
have examined the chemical and photochemical properties of molecular
oxygen on the (110) surface of rutile TiO<sub>2</sub> at 100 K using
electron energy loss spectroscopy (EELS), photon stimulated desorption
(PSD), and scanning tunneling microscopy (STM). Oxygen chemisorbs
on the TiO<sub>2</sub>(110) surface at 100 K through charge transfer
from surface Ti<sup>3+</sup> sites. The charge-transfer process is
evident in EELS by a decrease in the intensity of the Ti<sup>3+</sup> d-to-d transition at ∼0.9 eV and formation of a new loss
at ∼2.8 eV. On the basis of comparisons with the available
homogeneous and heterogeneous literature for complexed/adsorbed O<sub>2</sub>, the species responsible for the 2.8 eV peak can be assigned
to a surface peroxo (O<sub>2</sub><sup>2–</sup>) state of O<sub>2</sub>. This species was identified as the active form of adsorbed
O<sub>2</sub> on TiO<sub>2</sub>(110) for PSD. The adsorption site
of this peroxo species was assigned to that of a regular five-coordinated
Ti<sup>4+</sup> (Ti<sub>5c</sub>) site based on comparisons between
the UV exposure-dependent behavior of O<sub>2</sub> in STM, PSD, and
EELS data. Assignment of the active form of adsorbed O<sub>2</sub> to a peroxo species at normal Ti<sub>5c</sub> sites necessitates
reevaluation of the simple mechanism in which a single valence band
hole neutralizes a singly charged O<sub>2</sub> species (superoxo
or O<sub>2</sub><sup>–</sup>), leading to desorption of O<sub>2</sub> from a physisorbed potential energy surface
Deprotonated Water Dimers: The Building Blocks of Segmented Water Chains on Rutile RuO 2
Diffusion and Photon-Stimulated Desorption of CO on TiO<sub>2</sub>(110)
Thermal
diffusion of CO adsorbed on rutile TiO<sub>2</sub>(110)
was studied in the 20–110 K range using photon-stimulated desorption
(PSD), temperature-programmed desorption (TPD), and scanning tunneling
microscopy. During UV irradiation, CO desorbs from certain photoactive
sites (e.g., oxygen vacancies). This phenomenon was exploited to study
CO thermal diffusion in three steps: first, empty these sites during
a first irradiation cycle, then replenish them with CO during annealing,
and finally probe the active site occupancy in the second PSD cycle.
The PSD and TPD experiments show that the CO diffusion rate correlates
with the CO adsorption energystronger binding corresponds
to slower diffusion. Increasing the CO coverage from 0.06 to 0.44
monolayer (ML) or hydroxylation of the surface decreases the CO binding
and increases the CO diffusion rate. Relative to the reduced surface,
the CO adsorption energy increases and the diffusion decreases on
the oxidized surface. The CO diffusion kinetics can be modeled satisfactorily
as an Arrhenius process with a “normal” prefactor (i.e.,
ν = 10<sup>12</sup> s<sup>–1</sup>) and a Gaussian distribution
of activation energies where the peak of the distribution is ∼0.26
eV and the full width at half-maximum (fwhm) is ∼0.1 eV at
the lowest coverage. The observations are consistent with a significant
electrostatic component of the CO binding energy on the TiO<sub>2</sub>(110) surface which is affected by changes in the surface dipole
and dipole–dipole interactions
Deprotonated Water Dimers: The Building Blocks of Segmented Water Chains on Rutile RuO<sub>2</sub>(110)
Despite the importance of RuO<sub>2</sub> in photocatalytic water
splitting and catalysis in general, the interactions of water with
even its most stable (110) surface are not well understood. In this
study we employ a combination of high-resolution scanning tunneling
microscopy imaging with density functional theory based <i>ab
initio</i> molecular dynamics, and we follow the formation and
binding of linear water clusters on coordinatively unsaturated ruthenium
rows. We find that clusters of all sizes (dimers, trimers, tetramers,
extended chains) are stabilized by donating one proton per every two
water molecules to the surface bridge bonded oxygen sites, in contrast
with water monomers that do not show a significant propensity for
dissociation. The clusters with odd number of water molecules are
less stable than the clusters with even number and are generally not
observed under thermal equilibrium. For all clusters with even numbers,
the dissociated dimers represent the fundamental building blocks with
strong intradimer hydrogen bonds and only very weak interdimer interactions
resulting in segmented water chains
Light Makes a Surface Banana-Bond Split: Photodesorption of Molecular Hydrogen from RuO<sub>2</sub>(110)
The coordination of H<sub>2</sub> to a metal center via polarization
of its σ bond electron density, known as a Kubas complex, is
the means by which H<sub>2</sub> chemisorbs at Ru<sup>4+</sup> sites
on the rutile RuO<sub>2</sub>(110) surface. This distortion of electron
density off an interatomic axis is often described as a ‘banana-bond.’
We show that the Ru–H<sub>2</sub> banana-bond can be destabilized
and split using visible light. Photodesorption of H<sub>2</sub> (or
D<sub>2</sub>) is evident by mass spectrometry and scanning tunneling
microscopy. From time-dependent density functional theory, the key
optical excitation splitting the Ru–H<sub>2</sub> complex involves
an interband transition in RuO<sub>2</sub> which effectively diminishes
its Lewis acidity, thereby weakening the Kubas complex. Such excitations
are not expected to affect adsorbates on RuO<sub>2</sub> given its
metallic properties. Therefore, this common thermal cocatalyst employed
in photocatalysis is, itself, photoactive