0000000000299724

AUTHOR

G. Van Tendeloo

showing 4 related works from this author

Crystal structures of superconducting sodium intercalates of hafnium nitride chloride

2006

Sodium intercalation compounds of HfNCl have been prepared at room temperature in naphtyl sodium solutions in tetrahydrofuran and their crystal structure has been investigated by Rietveld refinement using X-ray powder diffraction data and high-resolution electron microscopy. The structure of two intercalates with space group Rm and lattice parameters a = 3.58131(6) A u , c = 57.752(6) A u , and a = 3.58791(8) A u , c = 29.6785(17) A u is reported, corresponding to the stages 2 and 1, respectively, of NaxHfNCl. For the stage 2 phase an ordered model is presented, showing two crystallographically independent (HfNCl) units with an alternation of the Hf-Hf interlayer distance along the c-axis, …

Materials scienceRietveld refinementMechanical EngineeringSodiumchemistry.chemical_elementSpace groupCrystal structureNitrideCondensed Matter PhysicsCrystalCrystallographychemistryMechanics of MaterialsX-ray crystallographyGeneral Materials SciencePowder diffractionMaterials Research Bulletin
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In situ study of the phase transition in Bi2Ti4O11

1995

Abstract The paraelectric ⇌ antiferroelectric phase transition of the compound Bi 2 Ti 4 O 11 is studied in situ by electron diffraction and electron microscopy. The transition is reversible and clearly second order. Above T c faint streaking at the superlattice positions persists. In the low-temperature phase, antiphase boundaries with a displacement vector R = 1/2[101] are revealed; they show a finite width, suggesting a gradual displacement of the Bi atoms at the transition. A model for the domain wall configuration is proposed, based on the influence of the lone pairs of Bi 3+ ions at the transition.

Phase transitionChemistrySuperlatticeCondensed Matter PhysicsMolecular physicsElectronic Optical and Magnetic MaterialsIonInorganic ChemistryCondensed Matter::Materials ScienceCrystallographyDomain wall (magnetism)Electron diffractionPhase (matter)Materials ChemistryCeramics and CompositesAntiferroelectricityPhysical and Theoretical ChemistryLone pairJournal of Solid State Chemistry
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Surface enhanced Raman scattering of silver sensitized cobalt nanoparticles in metal–dielectric nanocomposites

2008

We report the preparation of a new type of nanocomposite containing cobalt and silver nanoparticles organized in parallel layers with a well controlled separation. This arrangement allows the observation of an enhanced low-frequency Raman signal at the vibration frequency of cobalt nanoparticles excited through the surface plasmons of silver nanoparticles. Numerical simulations of the electric field confirm the emergence of hot spots when the separation between silver and cobalt nanoparticles is small enough. © IOP Publishing Ltd.

inorganic chemicalsMaterials scienceAnalytical chemistry[ PHYS.COND.CM-MS ] Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]chemistry.chemical_elementNanoparticleNanoprobeBioengineering02 engineering and technology01 natural sciencesSilver nanoparticlesymbols.namesake0103 physical sciencesGeneral Materials ScienceElectrical and Electronic Engineering010306 general physicsNanocompositeMechanical EngineeringPhysicsSurface plasmonGeneral Chemistry021001 nanoscience & nanotechnologychemistryChemical engineeringMechanics of Materialssymbols[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]0210 nano-technologyRaman spectroscopyCobaltRaman scattering
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Crystal structure of Bi_{6}Sr_{8-x}Ca_{3+x}O_{22}(-0.5\leq x\leq1.7)$: a mixed valence bismuth oxide related to perovskite

1998

Abstract: The crystal structure of BiSr8-xCa3+xO22 has been determined by single-crystal X-ray diffraction. This phase is the same as Bi9Sr11Ca5Oy that was previously studied by several authors as a secondary phase in the Bi-Sr-Ca-Cu-O system and coexists in thermodynamic equilibrium with the superconductors Bi2Sr2CuO6 and Bi2Sr2CaCu2O8 It crystallizes in the monoclinic space group P2(1)/c, with cell parameters a 11.037(3) Angstrom, b = 5.971(2) Angstrom, c = 19.703(7) Angstrom, beta = 101.46(3)degrees Z = 2. The structure was solved by direct methods and full-matrix least-squares refinement. It is built up by perovskite-related blocks of composition [Sr8-xBi2Ca3+xO16] that intergrow with d…

Materials scienceValence (chemistry)General Chemical EngineeringZone axisPhysicschemistry.chemical_elementGeneral ChemistryCrystal structureBismuthCrystallographyChemistrychemistryX-ray crystallographyMaterials ChemistryMonoclinic crystal systemSolid solutionPerovskite (structure)Chemistry of materials
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