4 research outputs found
Role of Cation–Water Disorder during Cation Exchange in Small-Pore Zeolite Sodium Natrolite
By
combining X-ray diffraction with oxygen K-edge absorption spectroscopy
we track changes occurring during the K<sup>+</sup>–Na<sup>+</sup> cation exchange of Na-natrolite (Na-NAT) as tightly bonded
Na<sup>+</sup> cations and H<sub>2</sub>O molecules convert into a
disordered K<sup>+</sup>–H<sub>2</sub>O substructure and the
unit cell expands by ca. 10% after 50% cation exchange. The coordination
of the confined H<sub>2</sub>O and nonframework cations change from
a tetrahedral configuration, similar in ice <i>I</i><sub><i>h</i></sub>, with Na<sup>+</sup> near the middle of
the channels in Na-NAT to two-bonded configuration, similar in bulk
water, and K<sup>+</sup> located near the walls of the framework in
K-NAT. This is related to the enhanced ion-exchange properties of
K-NAT, which, in marked contrast to Na-NAT, permits the exchange of
K<sup>+</sup> by a variety of uni-, di-, and trivalent cations
Spontaneous Ionic Polarization in Ammonia-Based Ionic Liquid
Ionic
liquids and gels have attracted attention for a variety of energy
storage applications, as well as for high-performance electrolytes
for batteries and supercapacitors. Although the electronic structure
of ionic electrolytes in these applications is of practical importance
for device design and improved performance, the understanding of the
electronic structure of ionic liquids and gels is still at an early
stage. Here we report soft X-ray spectroscopic measurements of the
surface electronic structure of a representative ammonia-based ionic
gel (DEME-TFSI with PS-PMMA-PS copolymer). We observe that, near the
outermost surface, the area of the anion peak (1s N<sup>–</sup> core level in TFSI) is relatively larger than that of the cation
peak (N<sup>+</sup> in DEME). This spontaneous ionic polarization
of the electrolyte surface, which is absent for the pure ionic liquid
without copolymer, can be directly tuned by the copolymer content
in the ionic gel, and further results in a modulation in work function.
These results shed new light on the control of surface electronic
properties of ionic electrolytes, as well as a difference between
their implementation in ionic liquids and gels
Atomically Engineered Metal–Insulator Transition at the TiO<sub>2</sub>/LaAlO<sub>3</sub> Heterointerface
We demonstrate that the atomic boundary
conditions of
simple binary
oxides can be used to impart dramatic changes of state. By changing
the substrate surface termination of LaAlO<sub>3</sub> (001) from
AlO<sub>2</sub> to LaO, the room-temperature sheet conductance of
anatase TiO<sub>2</sub> films are increased by over 3 orders of magnitude,
transforming the intrinsic insulating state to a high mobility metallic
state, while maintaining excellent optical transparency
Resolution of Electronic and Structural Factors Underlying Oxygen-Evolving Performance in Amorphous Cobalt Oxide Catalysts
Non-noble-metal,
thin-film oxides are widely investigated as promising
catalysts for oxygen evolution reactions (OER). Amorphous cobalt oxide
films electrochemically formed in the presence of borate (CoBi) and
phosphate (CoPi) share a common cobaltate domain building block, but
differ significantly in OER performance that derives from different
electron–proton charge transport properties. Here, we use a
combination of L edge synchrotron X-ray absorption (XAS), resonant
X-ray emission (RXES), resonant inelastic X-ray scattering (RIXS),
resonant Raman (RR) scattering, and high-energy X-ray pair distribution
function (PDF) analyses that identify electronic and structural factors
correlated to the charge transport differences for CoPi and CoBi.
The analyses show that CoBi is composed primarily of cobalt in octahedral
coordination, whereas CoPi contains approximately 17% tetrahedral
CoÂ(II), with the remainder in octahedral coordination. Oxygen-mediated
4<i>p</i>–3<i>d</i> hybridization through
Co–O–Co bonding was detected by RXES and the intersite <i>dd</i> excitation was observed by RIXS in CoBi, but not in CoPi.
RR shows that CoBi resembles a disordered layered LiCoO<sub>2</sub>-like structure, whereas CoPi is amorphous. Distinct domain models
in the nanometer range for CoBi and CoPi have been proposed on the
basis of the PDF analysis coupled to XAS data. The observed differences
provide information on electronic and structural factors that enhance
oxygen evolving catalysis performance