4 research outputs found
Visible Light Photo-oxidation of Model Pollutants Using CaCu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub>: An Experimental and Theoretical Study of Optical Properties, Electronic Structure, and Selectivity
Charge transfer between metal ions occupying distinct crystallographic sublattices in an ordered material is a strategy to confer visible light absorption on complex oxides to generate potentially catalytically active electron and hole charge carriers. CaCu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub> has distinct octahedral Ti<sup>4+</sup> and square planar Cu<sup>2+</sup> sites and is thus a candidate material for this approach. The solâgel synthesis of high surface area CaCu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub> and investigation of its optical absorption and photocatalytic reactivity with model pollutants are reported. Two gaps of 2.21 and 1.39 eV are observed in the visible region. These absorptions are explained by LSDA+U electronic structure calculations, including electron correlation on the Cu sites, as arising from transitions from a Cu-hybridized O 2p-derived valence band to localized empty states on Cu (attributed to the isolation of CuO<sub>4</sub> units within the structure of CaCu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub>) and to a Ti-based conduction band. The resulting charge carriers produce selective visible light photodegradation of 4-chlorophenol (monitored by mass spectrometry) by Pt-loaded CaCu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub> which is attributed to the chemical nature of the photogenerated charge carriers and has a quantum yield comparable with commercial visible light photocatalysts
Ion Dynamics and CO<sub>2</sub> Absorption Properties of Nbâ, Taâ, and YâDoped Li<sub>2</sub>ZrO<sub>3</sub> Studied by Solid-State NMR, Thermogravimetry, and First-Principles Calculations
Among
the many different processes proposed for large-scale carbon
capture and storage (CCS), high-temperature CO<sub>2</sub> looping
has emerged as a favorable candidate due to the low theoretical energy
penalties that can be achieved. Many different materials have been
proposed for use in such a process, the process requiring fast CO<sub>2</sub> absorption reaction kinetics as well as being able to cycle
the material for multiple cycles without loss of capacity. Lithium
ternary oxide materials, and in particular Li<sub>2</sub>ZrO<sub>3</sub>, have displayed promising performance, but further modifications
are needed to improve their rate of reaction with CO<sub>2</sub>.
Previous studies have linked rates of lithium ionic conduction with
CO<sub>2</sub> absorption in similar materials, and in this work we
present work aimed at exploring the effect of aliovalent doping on
the efficacy of Li<sub>2</sub>ZrO<sub>3</sub> as a CO<sub>2</sub> sorbent.
Using a combination of X-ray powder diffraction, theoretical calculations,
and solid-state nuclear magnetic resonance, we studied the impact
of Nb, Ta, and Y doping on the structure, Li ionic motion, and CO<sub>2</sub> absorption properties of Li<sub>2</sub>ZrO<sub>3</sub>. These
methods allowed us to characterize the theoretical and experimental
doping limit into the pure material, suggesting that vacancies formed
upon doping are not fully disordered but instead are correlated to
the dopant atom positions, limiting the solubility range. Characterization
of the lithium motion using variable-temperature solid-state nuclear
magnetic resonance confirms that interstitial doping with Y retards
the movement of Li ions in the structure, whereas vacancy doping with
Nb or Ta results in a similar activation energy as observed for nominally
pure Li<sub>2</sub>ZrO<sub>3</sub>. However, a marked reduction in
the CO<sub>2</sub> absorption of the Nb- and Ta-doped samples suggests
that doping also leads to a change in the carbonation equilibrium
of Li<sub>2</sub>ZrO<sub>3</sub>, disfavoring the CO<sub>2</sub> absorption
at the reaction temperature. This study shows that a complex mixture
of structural, kinetic, and dynamic factors can influence the performance
of Li-based materials for CCS and underscores the importance of balancing
these different factors in order to optimize the process
Control of Ionic Conductivity by Lithium Distribution in Cubic Oxide Argyrodites Li<sub>6+<i>x</i></sub>P<sub>1â<i>x</i></sub>Si<sub><i>x</i></sub>O<sub>5</sub>Cl
Argyrodite is a key structure type for ion-transporting
materials.
Oxide argyrodites are largely unexplored despite sulfide argyrodites
being a leading family of solid-state lithium-ion conductors, in which
the control of lithium distribution over a wide range of available
sites strongly influences the conductivity. We present a new cubic
Li-rich (>6 Li+ per formula unit) oxide argyrodite Li7SiO5Cl that crystallizes with an ordered cubic
(P213) structure at room temperature,
undergoing a transition at 473 K to a Li+ site disordered F4Ì
3m structure, consistent with
the symmetry adopted by superionic sulfide argyrodites. Four different
Li+ sites are occupied in Li7SiO5Cl (T5, T5a, T3, and T4), the combination of which is previously
unreported for Li-containing argyrodites. The disordered F4Ì
3m structure is stabilized to room temperature
via substitution of Si4+ with P5+ in Li6+xP1âxSixO5Cl (0.3 x < 0.85) solid solution. The resulting delocalization
of Li+ sites leads to a maximum ionic conductivity of 1.82(1)
Ă 10â6 S cmâ1 at x = 0.75, which is 3 orders of magnitude higher than the
conductivities reported previously for oxide argyrodites. The variation
of ionic conductivity with composition in Li6+xP1âxSixO5Cl is directly connected to structural changes
occurring within the Li+ sublattice. These materials present
superior atmospheric stability over analogous sulfide argyrodites
and are stable against Li metal. The ability to control the ionic
conductivity through structure and composition emphasizes the advances
that can be made with further research in the open field of oxide
argyrodites
Bi<sub>4</sub>O<sub>4</sub>Cu<sub>1.7</sub>Se<sub>2.7</sub>Cl<sub>0.3</sub>: Intergrowth of BiOCuSe and Bi<sub>2</sub>O<sub>2</sub>Se Stabilized by the Addition of a Third Anion
Layered
two-anion compounds are of interest for their diverse electronic
properties. The modular nature of their layered structures offers
opportunities for the construction of complex stackings used to introduce
or tune functionality, but the accessible layer combinations are limited
by the crystal chemistries of the available anions. We present a layered
three-anion material, Bi<sub>4</sub>O<sub>4</sub>Cu<sub>1.7</sub>Se<sub>2.7</sub>Cl<sub>0.3</sub>, which adopts a new structure type composed
of alternately stacked BiOCuSe and Bi<sub>2</sub>O<sub>2</sub>Se-like
units. This structure is accessed by inclusion of three chemically
distinct anions, which are accommodated by aliovalently substituted
Bi<sub>2</sub>O<sub>2</sub>Se<sub>0.7</sub>Cl<sub>0.3</sub> blocks
coupled to Cu-deficient Bi<sub>2</sub>O<sub>2</sub>Cu<sub>1.7</sub>Se<sub>2</sub> blocks, producing a formal charge modulation along
the stacking direction. The hypothetical parent phase Bi<sub>4</sub>O<sub>4</sub>Cu<sub>2</sub>Se<sub>3</sub> is unstable with respect
to its charge-neutral stoichiometric building blocks. The complex
layer stacking confers excellent thermal properties upon Bi<sub>4</sub>O<sub>4</sub>Cu<sub>1.7</sub>Se<sub>2.7</sub>Cl<sub>0.3</sub>: a
room-temperature thermal conductivity (Îș) of 0.4(1) W/mK was
measured on a pellet with preferred crystallite orientation along
the stacking axis, with perpendicular measurement indicating it is
also highly anisotropic. This Îș value lies in the ultralow regime
and is smaller than those of both BiOCuSe and Bi<sub>2</sub>O<sub>2</sub>Se. Bi<sub>4</sub>O<sub>4</sub>Cu<sub>1.7</sub>Se<sub>2.7</sub>Cl<sub>0.3</sub> behaves like a charge-balanced semiconductor with
a narrow band gap. The chemical diversity offered by the additional
anion allows the integration of two common structural units in a single
phase by the simultaneous and coupled creation of charge-balancing
defects in each of the units