23 research outputs found
Three-Dimensional Valency Mapping in Ceria Nanocrystals
Using electron tomography combined with electron energy loss spectroscopy (EELS), we are able to map the valency of the Ce ions in CeO<sub>2ā<i>x</i></sub> nanocrystals in three dimensions. Our results show a clear facet-dependent reduction shell at the surface of ceria nanoparticles; {111} surface facets show a low surface reduction, whereas at {001} surface facets, the cerium ions are more likely to be reduced over a larger surface shell. Our generic tomographic technique allows a full 3D data cube to be reconstructed, containing an EELS spectrum in each voxel. This possibility enables a three-dimensional investigation of a plethora of material-specific physical properties such as valency, chemical composition, oxygen coordination, or bond lengths, triggering the synthesis of nanomaterials with improved properties
Exceptional Layered Ordering of Cobalt and Iron in Perovskites
Exceptional
Layered Ordering of Cobalt and Iron in
Perovskite
Atomic Structure of Quantum Gold Nanowires: Quantification of the Lattice Strain
Theoretical studies exist to compute the atomic arrangement in gold nanowires and the influence on their electronic behavior with decreasing diameter. Experimental studies, <i>e.g.</i>, by transmission electron microscopy, on chemically synthesized ultrafine wires are however lacking owing to the unavailability of suitable protocols for sample preparation and the stability of the wires under electron beam irradiation. In this work, we present an atomic scale structural investigation on quantum single crystalline gold nanowires of 2 nm diameter, chemically prepared on a carbon film grid. Using low dose aberration-corrected high resolution (S)TEM, we observe an inhomogeneous strain distribution in the crystal, largely concentrated at the twin boundaries and the surface along with the presence of facets and surface steps leading to a noncircular cross section of the wires. These structural aspects are critical inputs needed to determine their unique electronic character and their potential as a suitable catalyst material. Furthermore, electron-beam-induced structural changes at the atomic scale, having implications on their mechanical behavior and their suitability as interconnects, are discussed
Atomic Structure of Quantum Gold Nanowires: Quantification of the Lattice Strain
Theoretical studies exist to compute the atomic arrangement in gold nanowires and the influence on their electronic behavior with decreasing diameter. Experimental studies, <i>e.g.</i>, by transmission electron microscopy, on chemically synthesized ultrafine wires are however lacking owing to the unavailability of suitable protocols for sample preparation and the stability of the wires under electron beam irradiation. In this work, we present an atomic scale structural investigation on quantum single crystalline gold nanowires of 2 nm diameter, chemically prepared on a carbon film grid. Using low dose aberration-corrected high resolution (S)TEM, we observe an inhomogeneous strain distribution in the crystal, largely concentrated at the twin boundaries and the surface along with the presence of facets and surface steps leading to a noncircular cross section of the wires. These structural aspects are critical inputs needed to determine their unique electronic character and their potential as a suitable catalyst material. Furthermore, electron-beam-induced structural changes at the atomic scale, having implications on their mechanical behavior and their suitability as interconnects, are discussed
Atomic Structure of Defects in Anion-Deficient Perovskite-Based Ferrites with a Crystallographic Shear Structure
Crystallographic
shear (CS) planes provide a new structure-generation mechanism in
the anion-deficient perovskites containing lone-pair cations. Pb<sub>2</sub>Sr<sub>2</sub>Bi<sub>2</sub>Fe<sub>6</sub>O<sub>16</sub>,
a new <i>n</i> = 6 representative of the A<sub><i>n</i></sub>B<sub><i>n</i></sub>O<sub>3<i>n</i>ā2</sub> homologous series of the perovskite-based ferrites with the CS structure,
has been synthesized using the solid-state technique. The structure
is built of perovskite blocks with a thickness of four FeO<sub>6</sub> octahedra spaced by double columns of FeO<sub>5</sub> edge-sharing
distorted tetragonal pyramids, forming 1/2[110](101)<sub>p</sub> CS
planes (space group <i>Pnma</i>, <i>a</i> = 5.6690(2)
Ć
, <i>b</i> = 3.9108(1) Ć
, <i>c</i> =
32.643(1) Ć
). Pb<sub>2</sub>Sr<sub>2</sub>Bi<sub>2</sub>Fe<sub>6</sub>O<sub>16</sub> features a wealth of microstructural phenomena
caused by the flexibility of the CS planes due to the variable ratio
and length of the constituting fragments with {101}<sub>p</sub> and
{001}<sub>p</sub> orientation. This leads to the formation of āwavesā,
āhairpinsā, āĪ-shapedā defects,
and inclusions of the hitherto unknown layered anion-deficient perovskites
Bi<sub>2</sub>(Sr,Pb)ĀFe<sub>3</sub>O<sub>8.5</sub> and Bi<sub>3</sub>(Sr,Pb)ĀFe<sub>4</sub>O<sub>11.5</sub>. Using a combination of diffraction,
imaging, and spectroscopic transmission electron microscopy techniques
this complex microstructure was fully characterized, including direct
determination of positions, chemical composition, and coordination
number of individual atomic species. The complex defect structure
makes these perovskites particularly similar to the CS structures
in ReO<sub>3</sub>-type oxides. The flexibility of the CS planes appears
to be a specific feature of the Sr-based system, related to the geometric
match between the SrO perovskite layers and the {100}<sub>p</sub> segments
of the CS planes
Epitaxy-Enabled VaporāLiquidāSolid Growth of Tin-Doped Indium Oxide Nanowires with Controlled Orientations
Controlling the morphology of nanowires
in bottom-up synthesis
and assembling them on planar substrates is of tremendous importance
for device applications in electronics, photonics, sensing and energy
conversion. To date, however, there remain challenges in reliably
achieving these goals of orientation-controlled nanowire synthesis
and assembly. Here we report that growth of planar, vertical and randomly
oriented tin-doped indium oxide (ITO) nanowires can be realized on
yttria-stabilized zirconia (YSZ) substrates via the epitaxy-assisted
vaporāliquidāsolid (VLS) mechanism, by simply regulating
the growth conditions, in particular the growth temperature. This
robust control on nanowire orientation is facilitated by the small
lattice mismatch of 1.6% between ITO and YSZ. Further control of the
orientation, symmetry and shape of the nanowires can be achieved by
using YSZ substrates with (110) and (111), in addition to (100) surfaces.
Based on these insights, we succeed in growing regular arrays of planar
ITO nanowires from patterned catalyst nanoparticles. Overall, our
discovery of unprecedented orientation control in ITO nanowires advances
the general VLS synthesis, providing a robust epitaxy-based approach
toward rational synthesis of nanowires
Ultrasmall CoO(OH)<sub><i>x</i></sub> Nanoparticles As a Highly Efficient āTrueā Cocatalyst in Porous Photoanodes for Water Splitting
The coupling of light absorbers to
cocatalysts with well-designed
optical and catalytic properties is of fundamental importance for
the development of efficient photoelectrocatalytic devices for solar-driven
water splitting. We achieved an effective loading of visible-light-active
porous hybrid photoanodes for water photooxidation with ultrasmall
(ā¼1ā2 nm), highly disordered CoOĀ(OH)<sub><i>x</i></sub> nanoparticles using a two-step impregnation method. Under
visible light (Ī» > 420 nm) irradiation, the resulting photoanodes
significantly outperformed photoanodes loaded with conventional cobalt-based
cocatalyst (Co-Pi) comprising larger nanoparticles (ā¼5 nm)
in terms of both Faradaic efficiency of oxygen evolution (by the factor
of 2) and performance stability under long-term irradiation. A combination
of STEM, XAS, cyclic voltammetry, and photoelectrochemical techniques
was used to elucidate the advantages of using ultrasmall CoOĀ(OH)<sub><i>x</i></sub> nanoparticles as cocatalysts. Specifically,
due to the high transparency of ultrasmall CoOĀ(OH)<sub><i>x</i></sub> nanoparticles in the visible range, higher loading of porous
photoanodes with cobalt catalytic sites can be achieved, while the
photocurrent losses due to parasitic light absorption by the cocatalyst
are minimized. Notably, a significant enhancement in stability of
ultrasmall CoOĀ(OH)<sub><i>x</i></sub> nanoparticles in borate
electrolytes as compared to phosphate electrolytes has been observed.
EXAFS data recorded before and after photoelectrocatalysis indicated
that the effect of the electrolyte on the stability can be explained
by the difference in structural ordering dictated by different interaction
of the electrolyte anions with cobalt ions, as corroborated by DFT
calculations. This study highlights the strong impact of structural
and optical properties of cocatalysts as well as the strong influence
of the electrolyte composition on the activity and stability of photoelectrocatalytic
systems comprising transition metal oxide electrocatalysts
Toward Deep Blue Nano Hope Diamonds: Heavily Boron-Doped Diamond Nanoparticles
The production of boron-doped diamond nanoparticles enables the application of this material for a broad range of fields, such as electrochemistry, thermal management, and fundamental superconductivity research. Here we present the production of highly boron-doped diamond nanoparticles using boron-doped CVD diamond films as a starting material. In a multistep milling process followed by purification and surface oxidation we obtained diamond nanoparticles of 10ā60 nm with a boron content of approximately 2.3 Ć 10<sup>21</sup> cm<sup>ā3</sup>. Aberration-corrected HRTEM reveals the presence of defects within individual diamond grains, as well as a very thin nondiamond carbon layer at the particle surface. The boron K-edge electron energy-loss near-edge fine structure demonstrates that the B atoms are tetrahedrally embedded into the diamond lattice. The boron-doped diamond nanoparticles have been used to nucleate growth of a boron-doped diamond film by CVD that does not contain an insulating seeding layer
Evidence for MetalāSupport Interactions in Au Modified TiO<sub><i>x</i></sub>/SBA-15 Materials Prepared by Photodeposition
Gold nanoparticles have been efficiently
photodeposited onto titanate-loaded
SBA-15 (TiĀ(<i>x</i>)/SBA-15) with different titania coordination.
Transmission electron microscopy shows that relatively large Au nanoparticles
are photodeposited on the outer surface of the TiĀ(<i>x</i>)/SBA-15 materials and that TiO<sub><i>x</i></sub> tends
to form agglomerates in close proximity to the Au nanoparticles, often
forming coreāshell Au/TiO<sub><i>x</i></sub> structures.
This behavior resembles typical processes observed due to strong-metal
support interactions. In the presence of gold, the formation of hydrogen
on TiĀ(<i>x</i>)/SBA-15 during the photodeposition process
and the performance in the hydroxylation of terephthalic acid is greatly
enhanced. The activity of the Au/TiĀ(<i>x</i>)/SBA-15 materials
is found to depend on the TiO<sub><i>x</i></sub> loading,
increasing with a larger amount of initially isolated TiO<sub>4</sub> tetrahedra. Samples with initially clustered TiO<sub><i>x</i></sub> species show lower photocatalytic activities. When isolated
zinc oxide (ZnO<sub><i>x</i></sub>) species are present
on TiĀ(<i>x</i>)/SBA-15, gold nanoparticles are smaller and
well dispersed within the pores. Agglomeration of TiO<sub><i>x</i></sub> species and the formation of Au/TiO<sub><i>x</i></sub> structures is negligible. The dispersion of gold
and the formation of Au/TiO<sub><i>x</i></sub> in the SBA-15
matrix seem to depend on the mobility of the TiO<sub><i>x</i></sub> species. The mobility is determined by the initial degree
of agglomeration of TiO<sub><i>x</i></sub>. Effective hydrogen
evolution requires Au/TiO<sub><i>x</i></sub> coreāshell
composites as in Au/TiĀ(<i>x</i>)/SBA-15, whereas hydroxylation
of terephthalic acid can also be performed with Au/ZnO<sub><i>x</i></sub>/TiO<sub><i>x</i></sub>/SBA-15 materials.
However, isolated TiO<sub><i>x</i></sub> species have to
be grafted onto the support prior to the zinc oxide species, providing
strong evidence for the necessity of TiāOāSi bridges
for high photocatalytic activity in terephthalic acid hydroxylation
Pyramid-Shaped Wurtzite CdSe Nanocrystals with Inverted Polarity
We report on pyramid-shaped wurtzite cadmium selenide (CdSe) nanocrystals (NCs), synthesized by hot injection in the presence of chloride ions as shape-directing agents, exhibiting reversed crystal polarity compared to former reports. Advanced transmission electron microscopy (TEM) techniques (image-corrected high-resolution TEM with exit wave reconstruction and probe-corrected high-angle annular dark field-scanning TEM) unequivocally indicate that the triangular base of the pyramids is the polar (0001Ģ
) facet and their apex points toward the [0001] direction. Density functional theory calculations, based on a simple model of binding of Cl<sup>ā</sup> ions to surface Cd atoms, support the experimentally evident higher thermodynamic stability of the (0001Ģ
) facet over the (0001) one conferred by Cl<sup>ā</sup> ions. The relative stability of the two polar facets of wurtzite CdSe is reversed compared to previous experimental and computational studies on Cd chalcogenide NCs, in which no Cl-based chemicals were deliberately used in the synthesis or no Cl<sup>ā</sup> ions were considered in the binding models. Self-assembly of these pyramids in a peculiar clover-like geometry, triggered by the addition of oleic acid, suggests that the basal (polar) facet has a density and perhaps type of ligands significantly different from the other three facets, since the pyramids interact with each other exclusively <i>via</i> their lateral facets. A superstructure, however with no long-range order, is observed for clovers with their (0001Ģ
) facets roughly facing each other. The CdSe pyramids were also exploited as seeds for CdS pods growth, and the peculiar shape of the derived branched nanostructures clearly arises from the inverted polarity of the seeds