Search results for "Reflection high-energy electron diffraction"

showing 10 items of 35 documents

Intrinsic nanostructures on the (001) surface of strontium titanate at low temperatures

2020

Atomically smooth (001) surfaces of SrTiO3 cut from the high-quality single crystals at two different miscut angles 0.9 and 7.0 deg between the real flat surfaces and crystallographic planes (001) were analyzed by means of the reflection high energy electron diffraction (RHEED) method from the room down to liquid helium temperatures. The diffraction patterns typical of the RHEED geometry close to ideal for a small miscut angle and those exhibiting distinct features of the specific periodicity associated with regular steps, which form due to the larger miscut angle, are presented. The surface symmetry and energetics were shown to impose differences in lattice parameters in parallel to a surf…

010302 applied physicsDiffractionMaterials scienceNanostructureReflection high-energy electron diffractionPhysics and Astronomy (miscellaneous)Condensed matter physicsGeneral Physics and Astronomy01 natural sciencesCondensed Matter::Materials Sciencesymbols.namesakechemistry.chemical_compoundchemistryElectron diffractionLattice (order)0103 physical sciencessymbolsStrontium titanate010306 general physicsRaman spectroscopySingle crystalLow Temperature Physics
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Reactivity of H2S and H2S/H2 Mixture With Molybdenum Oxide Thin Films Epitaxied on CoO (100) : Characterization by Rheed and Auger Spectroscopy

2010

Molybdenum-Cobalt composite oxide films were prepared by the evaporation of molybdenum trioxide on a fresh cleaved CoO (100) surface (Thickness = 10 A). The MoO3-CoO interface has been characterized simultaneously by reflexion high electron diffraction (RHEED) and Auger Electron Spectroscopy (AES). The thin film structure and composition depend on the annealing temperature. After a 300°C treatment, metallic cobalt islands nucleate at the interface thin film - CoO (100) and crystallize with the cubic FCC symmetry. After a 700°C treatment cobalt molybdate (a CoMoO4) islands grow. The metastable crystallites are epitaxied on CoO (100). After a 900°C treatment, the thin film consists of flat tw…

Auger electron spectroscopyCrystallographychemistry.chemical_compoundReflection high-energy electron diffractionChemistrychemistry.chemical_elementGeneral ChemistryCrystalliteThin filmMolybdateCobaltAmorphous solidMolybdenum trioxideBulletin des Sociétés Chimiques Belges
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Effect of the surface stoichiometry on the interaction of Mo with TiO2 (110)

2000

Abstract Molydenum has been deposited at room temperature on (110) TiO2 surfaces with different stoichiometries, roughnesses and crystallinities. Whatever the substrate preparation is, in-situ Auger electron spectroscopy (AES) and X-ray photoelectron spectroscopy (XPS) studies as well as ex-situ atomic force microscopy (AFM) and reflexion high-energy electron diffraction (RHEED) studies reveal a Stranski–Krastanov growth mode: the completion of three monolayers followed by islands growth is observed in every case. The three monolayers are always composed of amorphous molybdenum oxide with an oxidation state of molybdenum less than IV. The oxidation of the molybdenum layers generates Ti3+ an…

Auger electron spectroscopyReflection high-energy electron diffractionChemistryAnalytical chemistrychemistry.chemical_elementSurfaces and InterfacesSubstrate (electronics)Condensed Matter PhysicsElectron beam physical vapor depositionSurfaces Coatings and FilmsCrystallographyX-ray photoelectron spectroscopyElectron diffractionMolybdenumMonolayerMaterials ChemistrySurface Science
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Size-dependent alignment of Fe nanoparticles upon deposition onto W(110)

2010

Using in situ electron diffraction we study the orientation of mass-selected iron nanoparticles upon deposition onto single crystalline W(110) at room temperature. It is found that particles with a diameter below about 4 nm and a kinetic energy $\ensuremath{\le}0.1$ electron volt per atom spontaneously align with respect to the substrate. Larger particles preferentially rest with their (001) and (110) facets parallel to the surface, but do not show further alignment. The data may hint at thermally activated dislocation motions upon the impact on the substrate which are responsible for the observed orientation below 4 nm. By this uniformly oriented monodisperse nanostructures can be prepared…

CrystallographyNanostructureReflection high-energy electron diffractionMaterials scienceElectron diffractionAtomNanoparticleSubstrate (electronics)DislocationCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsElectron backscatter diffractionPhysical Review B
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Using Electron Diffraction to Solve the Crystal Structure of a Laked Azo Pigment

2009

The structure of the ζ phase of Pigment Red 53:2 was solved using electron diffraction data. The unit cell determination appeared to be more complicated due to twinning of the crystals. A series of...

DiffractionCrystallographyReflection high-energy electron diffractionElectron diffractionGas electron diffractionChemistryGeneral Materials ScienceGeneral ChemistryCrystal structureCondensed Matter PhysicsCrystal twinningCrystallographic defectElectron backscatter diffractionCrystal Growth & Design
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Electron diffraction, X-ray powder diffraction and pair-distribution-function analyses to determine the crystal structures of Pigment Yellow 213, C23…

2009

The crystal structure of the nanocrystalline alpha phase of Pigment Yellow 213 (P.Y. 213) was solved by a combination of single-crystal electron diffraction and X-ray powder diffraction, despite the poor crystallinity of the material. The molecules form an efficient dense packing, which explains the observed insolubility and weather fastness of the pigment. The pair-distribution function (PDF) of the alpha phase is consistent with the determined crystal structure. The beta phase of P.Y. 213 shows even lower crystal quality, so extracting any structural information directly from the diffraction data is not possible. PDF analysis indicates the beta phase to have a columnar structure with a si…

DiffractionModels MolecularAza CompoundsReflection high-energy electron diffractionChemistryMolecular ConformationGeneral MedicineCrystal structurePair-distribution functionHeterocyclic Compounds 4 or More RingsGeneral Biochemistry Genetics and Molecular BiologyPigment Yellow 213CrystalCrystallinityCrystallographyElectron diffractionElectron diffractionMicroscopy Electron TransmissionX-ray powder diffractionElectron diffraction; Pair-distribution function; Pigment Yellow 213; X-ray powder diffractionParticle SizeColoring AgentsPowder diffractionPowder DiffractionElectron backscatter diffractionActa crystallographica. Section B, Structural science
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Cooperative atomic motion probed by ultrafast transmission electron diffraction

2015

In numerous solids exhibiting broken symmetry ground states, changes in electronic (spin) structure are accompanied by structural changes. Femtosecond time-resolved techniques recently contributed many important insights into the origin of their ground states by tracking dynamics of the electronic subsystem with femtosecond light pulses. Moreover, several studies of structural dynamics in systems with periodic lattice modulation (PLD) were performed. Since intensities of the super-lattice diffraction peaks are in the first approximation proportional to the square of the PLD amplitude, their temporal dynamics provides access to cooperative atomic motion. This process takes place on a fractio…

DiffractionPhysicsOpticsReflection high-energy electron diffractionElectron diffractionbusiness.industryLattice (order)SuperlatticeExcited stateFemtosecondElectronbusinessMolecular physicsSPIE Proceedings
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The role of electron diffraction in zeolite structure determination

2006

Because electron diffraction can sample individual microcrystals, it is clear that this single crystal method can facilitate, in at least two ways, structure determination for inorganic materials, such as zeolites, that are preferentially microcrystalline. First, in a qualitative application, three-dimensional tilts of individual small crystals, to map the reciprocal lattice, greatly facilitates unit cell and space group determination when powder diffraction indexing programs fail. If incoherent multiple scattering leads to violation of systematic absences, these absences can be restored by collection of precession diffraction patterns based on the Vincent-Midgley method [1], as demonstrate…

DiffractionReflection high-energy electron diffractionChemistryGas electron diffractionElectron crystallographybusiness.industrySayre equationMolecular physicsOpticsElectron diffractionStructural BiologyDirect methodsbusinessPowder diffractionActa Crystallographica Section A Foundations of Crystallography
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Automated electron diffraction tomography - a new tool for nano crystal structure analysis

2011

Automated electron Diffraction Tomography (ADT) comprises an upcoming method for “ab intio” structure analysis of nano crystals. ADT allows fine sampling of the reciprocal space by sequential collection of electron diffraction patterns while tilting a nano crystal in fixed tilt steps around an arbitrary axis. Electron diffraction is collected in nano diffraction mode (NED) with a semi-parallel beam with a diameter down to 50 nm. For crystal tracking micro-probe STEM imaging is used. Full automation of the acquisition procedure allowed optimisation of the electron dose distribution and therefore analysis of highly beam sensitive samples. Cell parameters, space group and reflection intensitie…

DiffractionReflection high-energy electron diffractionChemistrybusiness.industryGeneral ChemistryCondensed Matter Physicsstructure determinationCrystalReciprocal latticeOpticsreciprocal space tomographyElectron diffractionelectron diffraction; reciprocal space tomography; structure determinationelectron diffractionGeneral Materials ScienceDiffraction topographybusinessPowder diffractionElectron backscatter diffraction
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Elucidating structural order and disorder phenomena in mullite-type Al4B2O9 by automated electron diffraction tomography

2017

The crystal structure and disorder phenomena of Al4B2O9, an aluminum borate from the mullite-type family, were studied using automated diffraction tomography (ADT), a recently established method for collection and analysis of electron diffraction data. Al4B2O9, prepared by sol-gel approach, crystallizes in the monoclinic space group C2/m. The ab initio structure determination based on three-dimensional electron diffraction data from single ordered crystals reveals that edge-connected AlO6 octahedra expanding along the b axis constitute the backbone. The ordered structure (A) was confirmed by TEM and HAADF-STEM images. Furthermore, disordered crystals with diffuse scattering along the b axis…

DiffractionReflection high-energy electron diffractionMaterials scienceGas electron diffraction02 engineering and technologyCrystal structure010402 general chemistry021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciences0104 chemical sciencesElectronic Optical and Magnetic MaterialsInorganic ChemistryDiffraction tomographyCrystallographyElectron diffractionMaterials ChemistryCeramics and CompositesPhysical and Theoretical Chemistry0210 nano-technologySuperstructure (condensed matter)Electron backscatter diffractionJournal of Solid State Chemistry
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