Search results for "CONDENSED MATTER"

showing 10 items of 13918 documents

COMPARISON OF CPML IMPLEMENTATIONS FOR THE GPU-ACCELERATED FDTD SOLVER

2011

Three distinctively difierent implementations of convolu- tional perfectly matched layer for the FDTD method on CUDA enabled graphics processing units are presented. All implementations store ad- ditional variables only inside the convolutional perfectly matched lay- ers, and the computational speeds scale according to the thickness of these layers. The merits of the difierent approaches are discussed, and a comparison of computational performance is made using complex real-life benchmarks.

CUDAPerfectly matched layerScale (ratio)Computer scienceFinite-difference time-domain methodParallel computingGraphicsSolverCondensed Matter PhysicsImplementationElectronic Optical and Magnetic MaterialsComputational scienceProgress In Electromagnetics Research M
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Element-Selective Magnetic Imaging in Exchange-Coupled Systems by Magnetic Photoemission Microscopy

1998

We have used a photoemission microscope to obtain element-resolved magnetic contrast in stacked magnetic thin film systems. Magnetic information is thereby provided by X-ray magnetic circular dichroism. Elemental sensitivity, which is crucial for studying magnetic coupling phenomena in systems with several different layers, is achieved by tuning the energy of the illuminating photons to atomic absorption edges. We present measurements of a Ni-coated Co micropattern on Cu(001), and a wedged Co/Cr/Fe(001) sample. In the former sample the Ni magnetization is seen to follow the magnetization of the Co pattern, thereby changing from an out-of-plane easy axis in areas without underlying Co to in…

Materials scienceMagnetic domainMagnetic momentCondensed matter physicsMagnetic circular dichroismAnalytical chemistrySurfaces and InterfacesCondensed Matter PhysicsSurfaces Coatings and FilmsMagnetizationParamagnetismMagnetic anisotropyX-ray magnetic circular dichroismMaterials ChemistryMagnetic force microscopeSurface Review and Letters
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Preparation and crystal structure of the oxalato-bridged CrIII–AgItwo-dimensional compound {Ag3(H2O)[Cr(dpa)(ox)2]3}n·2nH2O (dpa = 2,2′-dipyridylamin…

2004

The reaction of the mononuclear complex [Cr(dpa)(ox)2]− (dpa = 2,2-dipyridylamine) with Ag+ in aqueous solution affords the two-dimensional compound {Ag3(H2O)[Cr(dpa)(ox)2]3}n·2nH2O (1) whose structure has been determined by single-crystal X-ray diffraction. Six crystallographically independent metal atoms (three chromium and three silver atoms) occur in 1. The three [Cr(dpa)(ox)2]− units in 1 act as ligands towards the silver atoms through the two oxalate groups. Each oxalate group acts as bridging ligand adopting five coordination modes: bis-bidentate, bis-bidentate/monodentate (outer), bis-bidentate/monodentate (inner), bidentate/bis-monodentate (outer) and bidentate/monodentate (outer).…

DenticityAqueous solutionInorganic chemistrychemistry.chemical_elementBridging ligandGeneral ChemistryCrystal structureCondensed Matter PhysicsBlock (periodic table)OxalateMetalCrystallographychemistry.chemical_compoundChromiumchemistryvisual_artvisual_art.visual_art_mediumGeneral Materials ScienceCrystEngComm
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Tenfold increase in efficiency from a reference blue OLED

2018

Abstract Starting from a reference single-layer light-emitting diode based on the blue phosphorescent bis-cyclometallated iridium complex FIrpic as guest, hosted in a PVK (non-conjugated poly(vynilcarbazole)) matrix, different strategies are followed to improve the efficiency of the devices through the combination of solution processed and evaporated layers. Injection of charges from the electrodes has been varied by using different conductive PEDOT: PSS as hole injection layer and a nanoscale Cs2CO3 interlayer as electron injection and hole-blocking film. Furthermore, a separated electron injection/hole blocking evaporated layer, TPBi or 3TPYMB, is introduced in double-layer devices to enh…

Materials sciencebusiness.industryBiophysicschemistry.chemical_element02 engineering and technologyGeneral ChemistryElectron010402 general chemistry021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesBiochemistryAtomic and Molecular Physics and Optics0104 chemical scienceschemistryPEDOT:PSSElectrodeOLEDOptoelectronicsIridium0210 nano-technologyPhosphorescencebusinessLayer (electronics)DiodeJournal of Luminescence
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Crystal structures, infrared-spectra, and thermal behavior of calcium hydrogenselenite monohydrate, Ca(HSeO3)2 · H2O, and dicalcium diselenite bis(hy…

1986

Abstract Calcium hydrogenselenite monohydrate and dicalcium diselenite bis(hydrogenselenite) were synthesized and their crystal structures determined. Crystal data for Ca(HSeO3)2 · H2O: a = 6.911(2), b = 7.369(2), c = 6.739(2) A, α = 90.51(3)°, β = 90.93(3)°, γ = 107.46(2)°, V = 327.3(2) A3, space group P 1 (No. 2), dcalcd = 3.19 M gm−3, Z = 2, and R = 0.036 for 1503 reflections. Data for Ca2(HSeO3)2(Se2O5): a = 14.719(4), b = 7.059(2), c = 11.793(2) A, β = 117.96(2)°, V = 1082.3(4) A3, space group C2 c (No. 15), dcalcd = 3.52 Mg m−3, Z = 4, and R = 0.047 for 1251 reflections. Both structures form a three-dimensional network. The coordination polyhedron around calcium is a monocapped trigon…

chemistry.chemical_classificationInfraredInfrared spectroscopychemistry.chemical_elementCrystal structureCalciumCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsInorganic ChemistryCrystallographyTrigonal prismchemistryCrystal dataX-ray crystallographyMaterials ChemistryCeramics and CompositesPhysical and Theoretical ChemistryInorganic compoundJournal of Solid State Chemistry
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Defects in yttrium aluminium perovskite and garnet crystals: atomistic study

2000

Native and impurity point defects in both yttrium aluminium perovskite (YAP) and garnet (YAG) crystals are studied in the framework of the pair-potential approximation coupled with the shell model description of the lattice ions. The calculated formation energies for native defects suggest that the antisite disorder is preferred over the Frenkel and Schottky-like disorder in both YAP and YAG. The calculated values of the distortion caused by the antisite YAl x in the lattice turn out to be in an excellent agreement with the EXAFS measurements. In non-stoichiometric compounds, the calculated reaction energies indicate that excess Y2 O3 or Al2 O3 is most likely to be accommodated by the forma…

Aluminium oxidesCrystallographyMaterials scienceExtended X-ray absorption fine structureImpurityYttrium aluminiumLattice (order)MineralogyGeneral Materials ScienceCondensed Matter PhysicsCrystallographic defectPerovskite (structure)IonJournal of Physics: Condensed Matter
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Hot electron effects in metallic single electron components

1996

Thermalisation of single electron devices is of considerable current interest because of its fundamental and practical consequences. We present experimental evidence of the effect of electrode volume and its shape on thermal equilibration of small metallic islands for single electron tunnelling. Heat transport between the conduction electrons and the lattice in a metal is commonly accepted to obey the ∝Te5-T0/5 law at low electron and lattice temperatures,Te andT0, respectively. We have investigated the power law and found that it obeys the ∝T5 law only for the smallest islands, and in the majority of the cases considered, it rather follows a law ∝Tp, wherep<5. The thermal coupling can be i…

Coupling constantMetalThermalisationMaterials scienceCondensed matter physicsvisual_artLattice (order)Electrodevisual_art.visual_art_mediumGeneral Physics and AstronomyElectronThermal conductionPower lawCzechoslovak Journal of Physics
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Electromagnetic behaviour of superconductive amorphous metals

2005

The penetration depth of the magnetic field into an amorphous superconductor is calculated. The ratio of the London penetration depth δL to the electron free path le under zero temperature is above unity for almost all amorphous metals. That is why pure metals, in a superconducting state, change from type I superconductors to type II superconductors during the crystalline–amorphous transition.

SuperconductivityMaterials scienceAmorphous metalCondensed matter physicsMean free pathLondon penetration depthCondensed Matter PhysicsCondensed Matter::Disordered Systems and Neural NetworksAmorphous solidCondensed Matter::Materials ScienceMeissner effectCondensed Matter::SuperconductivityGeneral Materials SciencePenetration depthType-II superconductorJournal of Physics: Condensed Matter
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Gradientenabhängigkeit der Viskosität verdünnter Lösungen von Fadenmolekülen

1964

Es wird uber die Gradientenabhangigkeit der Viskositat von Polymeren mit hohem Molekulargewicht in Losungsmitteln ublicher Viskositat berichtet. Die Ermittlung von [η] fur verschwindenden Gradienten [η]G→0 und besonders fur sehr hohe Gradienten [η]G→∞ wird diskutiert.

ChemistryPolymer chemistryGeneral Materials ScienceCondensed Matter PhysicsRheologica Acta
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Development of core-shell colloids to study self-diffusion in highly concentrated dispersions

2007

To study single particle motion in highly concentrated colloidal dispersions, a host-tracer colloid system was developed, consisting of crosslinked polymer micronetwork spheres placed in a good solvent. The host colloid is made invisible to the experimental probe by matching its refractive index to that of the solvent. For the tracer particles a core-shell structure was chosen to ensure the interaction potential to be identical to that of the host particles. Therefore the shell was made of the same polymer as the host. The core differs in refractive index from the solvent and is therefore visible due to scattered light.

chemistry.chemical_classificationQuantitative Biology::BiomoleculesSelf-diffusionMaterials scienceShell (structure)PolymerCondensed Matter::Soft Condensed MatterCore (optical fiber)ColloidchemistryDynamic light scatteringChemical physicsSPHERESRefractive index
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