Search results for "PEROVSKITE"

showing 10 items of 458 documents

Laser-Calorimetric Study of Fundamental Absorption Edge in Pb,La(ZrTi)O3 (PLZT) Perovskite Ceramics

2000

The values of the light absorption coefficient of PLZT 10/65/35 ceramics at selected wavelengths have been obtained by laser calorimetric measurements. The absorption coefficient of the PLZT ceramics is an exponential function of the photon energy. Two values of characteristic Urbach energy have been found ΔE1 = 106 meV and ΔE2 = 238 meV. The first one is a characteristic of the potential of electron-phonon interaction of the optically excited transitions from the valence band to the conduction band and does not depend on lattice defects or admixtures. The other characterises the electron-phonon interaction at optical transitions between two localized electron states in the energy gap separ…

Materials scienceAbsorption edgeBand gapAtomic electron transitionAbsorption bandExcited stateAttenuation coefficientMineralogyAtomic physicsPhoton energyPerovskite (structure)
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CO2 laser-induced structure changes in lead zirconate titanate Pb(Zr0.58Ti0.42)O3 sol–gel films

2003

Based on absorption spectra of lanthanum modified lead zirconate titanate Pb0.9La0.1(Zr0.65Ti0.35)O3 (PLZT10/65/35) ferroelectric ceramics an idea of local and selective treatment of lead zirconite titanate Pb(ZrXTi1−X)O3 (PZT) sol–gel film in the multi-layer structure by CO2 laser radiation was formulated. The possibility to obtain PZT perovskite film on the SiO2/Si substrate by irradiation with CO2 laser was shown experimentally. X-ray studies revealed the PZT perovskite structure ratio growth at the expenses of pirochlore structure with an increased power density of laser radiation.

Materials scienceAbsorption spectroscopyFerroelectric ceramicsGeneral Physics and Astronomychemistry.chemical_elementMineralogySurfaces and InterfacesGeneral ChemistryCondensed Matter PhysicsLead zirconate titanateLaserTitanateSurfaces Coatings and Filmslaw.inventionchemistry.chemical_compoundchemistrylawLanthanumComposite materialSol-gelPerovskite (structure)Applied Surface Science
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Room-Temperature Cubic Phase Crystallization and High Stability of Vacuum-Deposited Methylammonium Lead Triiodide Thin Films for High-Efficiency Sola…

2019

Methylammonium lead triiodide (MAPI) has emerged as a high-performance photovoltaic material. Common understanding is that at room temperature it adopts a tetragonal phase and it only converts to the perfect cubic phase around 50-60 ºC. Most MAPI films are prepared using a solution-based coating process, yet they can also be obtained by vapor phase deposition methods. Vapor phase processed MAPI films have significantly different characteristics compared to their solvent processed analogous, such as a relatively small crystal grain sizes and short excited state lifetimes. Yet solar cells based on vapor phase processed MAPI films exhibit high power conversion efficiencies. Surprisingly, after…

Materials scienceAnalytical chemistry02 engineering and technologyCubic crystal system010402 general chemistry7. Clean energy01 natural scienceslaw.inventionchemistry.chemical_compoundTetragonal crystal systemlawPhase (matter)Deposition (phase transition)General Materials ScienceThin filmTriiodideCrystallizationMaterialsCèl·lules fotoelèctriquesPerovskite (structure)Mechanical Engineering021001 nanoscience & nanotechnology0104 chemical scienceschemistryMechanics of Materials0210 nano-technology
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LPE growth and study of the Ce3+ incorporation in LuAlO3:Ce single crystalline film scintillators

2019

This work reports the results of the optical and electron paramagnetic resonance (EPR) investigation of the Ce3+ incorporation in single crystalline film (SCF) scintillators of Ce-doped LuAlO3 perovskite, grown by the liquid phase epitaxy method onto YAlO3 substrates using a PbO–B2O3 flux. The absorption, luminescence and EPR spectra showed the presence of the main Ce3+ center type (CeLu) corresponding to the location of Ce3+ ions in the twelve-fold coordinated cuboctahedral positions of the LuAlO3 host. Also the dimer CeLu–CeLu centers were found in the EPR spectra of the LuAP:Ce SCFs. No EPR spectrum of the Ce3+ ions located in the octahedral positions of Al3+ cations has been detected in…

Materials scienceAnalytical chemistry02 engineering and technologyGeneral Chemistry010402 general chemistry021001 nanoscience & nanotechnologyCondensed Matter PhysicsEpitaxy01 natural sciences0104 chemical scienceslaw.inventionIonOctahedronlawGeneral Materials ScienceAbsorption (chemistry)0210 nano-technologyElectron paramagnetic resonanceLuminescenceHyperfine structurePerovskite (structure)CrystEngComm
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Humidity-Induced Grain Boundaries in MAPbI3 Perovskite Films

2016

Methylammonium lead halide perovskites (MAPbI3) are very sensitive to humid environments. We performed in situ scanning force microscopy and in situ X-ray diffraction measurements on MAPbI3 films to track changes in the film morphology and crystal structure upon repeated exposure to a high relative humidity environment (80%). We found that the appearance of monohydrate (MAPbI3·H2O) Bragg reflections coincided with the appearance of additional grain boundaries. Prolonging the exposure time to humidity induced more grain boundaries and steps in the MAPbI3 films, and the peak intensities of the monohydrate MAPbI3·H2O increased. The monohydrate was not stable under dry atmosphere and could be r…

Materials scienceAnalytical chemistryHumidity02 engineering and technologyCrystal structureMethylammonium lead halide010402 general chemistry021001 nanoscience & nanotechnology01 natural sciences0104 chemical sciencesSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsAtmospherechemistry.chemical_compoundCrystallographyHysteresisGeneral EnergychemistryGrain boundaryRelative humidityPhysical and Theoretical Chemistry0210 nano-technologyPerovskite (structure)The Journal of Physical Chemistry C
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(La0.8Sr0.2)(Mn1−yFey)O3±δ oxides for ITSOFC cathode materials?

2005

The oxygen transport properties in (La 0.8 Sr 0.2 )(Mn 1-y Fe y )O 3±δ (LSMF) with various iron contents y = 0, 0.2, 0.5, 0.8 and 1 were determined by the IEDP technique. Both oxygen diffusion and surface exchange coefficients were found to be greater for y = 0.8 and 1 than those of LSM (y=0). Moreover, for y ≤0.5, grain boundary diffusion was the rate limiting step especially at lower temperatures. Thus, in the LSMF perovskite materials, the oxygen diffusion via oxygen vacancies is enhanced by Fe. The LSMF electrical performances were measured by impedance spectroscopy. Compared to LSM and LSF (y= 1), porous LSMF cathodes with y= 0.2-0.8 exhibit poor electronic conductivity: Fe, by reducin…

Materials scienceAnalytical chemistryOxygen transportMineralogychemistry.chemical_element02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnology01 natural sciences7. Clean energyOxygenCathode0104 chemical sciencesDielectric spectroscopylaw.inventionchemistryElectrical resistivity and conductivitylawMaterials ChemistryCeramics and CompositesIonic conductivityGrain boundary diffusion coefficient0210 nano-technologyPerovskite (structure)Journal of the European Ceramic Society
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Disorder-induced Raman scattering in rhenium trioxide (ReO3)

2007

Raman scattering in cubic metallic perovskite (ReO3) was studied at room temperature for well-crystallized monolith, polycrystalline powder and thin film samples. Defect-induced first-order Raman scattering was detected from the sub-surface region, given by the penetration depth of a 633 nm laser, and its origin was explained on the basis of a rigid-ion vibrational model for bulk ReO3. A quenching of the Raman intensity was observed in crystalline monolithic ReO3 upon increasing the temperature up to 250 °C and was related to crystal surface reconstruction/annealing.

Materials scienceAnnealing (metallurgy)Analytical chemistryMineralogyCondensed Matter PhysicsCrystalCondensed Matter::Materials Sciencesymbols.namesakechemistry.chemical_compoundRhenium trioxideX-ray Raman scatteringchemistryCondensed Matter::SuperconductivitysymbolsGeneral Materials SciencePenetration depthRaman spectroscopyRaman scatteringPerovskite (structure)Journal of Physics: Condensed Matter
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Dual-source vacuum deposition of pure and mixed halide 2D perovskites: thin film characterization and processing guidelines

2020

The dual-source vacuum deposition of 2D perovskite films of the type PEA2PbX4, (PEA = phenethylammonium and X = I−, Br−, or a combination of both) is presented. Low-temperature deposited 2D perovskite films showed high crystallinity with the expected trend of bandgap as a function of halide type and concentration. Importantly, we observed an unavoidable halide cross-contamination among different deposition runs, as well as a strong dependence of the material quality on the type of halide precursors used. These findings should be taken into account in the development of vacuum processing for low-dimensional mixed halide perovskites.

Materials scienceBand gapAnalytical chemistryHalide02 engineering and technologyGeneral Chemistry010402 general chemistry021001 nanoscience & nanotechnology01 natural sciences0104 chemical sciencesCharacterization (materials science)CrystallinityVacuum depositionSemiconductorsMaterials ChemistryDeposition (phase transition)Thin film0210 nano-technologyMaterialsPerovskite (structure)
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Efficient Wide-Bandgap Mixed-Cation and Mixed-Halide Perovskite Solar Cells by Vacuum Deposition

2021

Vacuum deposition methods are increasingly applied to the preparation of perovskite films and devices, in view of the possibility to prepare multilayer structures at low temperature. Vacuum-deposited, wide-bandgap solar cells based on mixed-cation and mixed-anion perovskites have been scarcely reported, due to the challenges associated with the multiple-source processing of perovskite thin films. In this work, we describe a four-source vacuum deposition process to prepare wide-bandgap perovskites of the type FA1-n Cs n Pb(I1-x Br x )3 with a tunable bandgap and controlled morphology, using FAI, CsI, PbI2, and PbBr2 as the precursors. The simultaneous sublimation of PbI2 and PbBr2 allows the…

Materials scienceBand gapEnergy Engineering and Power TechnologyHalide02 engineering and technology010402 general chemistry01 natural sciences7. Clean energyVacuum depositionMaterials ChemistryThin filmCèl·lules fotoelèctriquesPerovskite (structure)Range (particle radiation)Renewable Energy Sustainability and the Environmentbusiness.industryConductivitat elèctrica021001 nanoscience & nanotechnology0104 chemical sciencesFuel TechnologyChemistry (miscellaneous)HomogeneousOptoelectronicsPhotovoltaics and Wind EnergySublimation (phase transition)0210 nano-technologybusinessACS Energy Letters
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Vacuum-Deposited Multication Tin-Lead Perovskite Solar Cells

2020

The use of a combination of tin and lead is the most promising approach to fabricate narrow bandgap metal halide perovskites. This work presents the development of reproducible tin and lead perovskites by vacuum co-deposition of the precursors, a solvent-free technique which can be easily implemented to form complex stacks. Crystallographic and optical characterization reveal the optimal film composition based on cesium and methylammonium monovalent cations. Device optimization makes use of the intrinsically additive nature of vacuum deposition, resulting in solar cells with 8.89% photovoltaic efficiency. The study of the devices by impedance spectroscopy identifies bulk recombination as on…

Materials scienceBand gapEnergy Engineering and Power TechnologyHalidechemistry.chemical_element02 engineering and technology010402 general chemistry01 natural sciences7. Clean energylaw.inventionVacuum depositionlawSolar cellMaterials ChemistryElectrochemistryChemical Engineering (miscellaneous)Electrical and Electronic EngineeringMaterialsCèl·lules fotoelèctriquesPerovskite (structure)business.industryPhotovoltaic system021001 nanoscience & nanotechnology0104 chemical sciencesDielectric spectroscopychemistryOptoelectronics0210 nano-technologybusinessTin
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