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Impedance spectroscopy studies of SrMnO3, BaMnO3and Ba0.5Sr0.5MnO3ceramics

2014

The impedance spectrum of hexagonal SrMnO3, rhombohedral BaMnO3 and orthorhombic Ba0.5Sr0.5MnO3 ceramics, synthesized by conventional high-temperature method, was studied in a wide temperature and frequency range. The complex impedance plots of Z″ versus Z′ pointed to two contributions originating from grains and grain boundaries. The parameters of electric equivalent circuit were calculated. The semicircles related to the grain boundary are located at the lower frequency side due to higher resistivity and capacity of the grain boundaries. The Ba0.5Sr0.5MnO3 ceramics is characterized by the lowest activation energy related to the grains. The conductivities σac of all the investigated sample…

Materials scienceCondensed matter physicsMineralogyActivation energyConductivityDielectric spectroscopyElectrical resistivity and conductivityvisual_artvisual_art.visual_art_mediumGeneral Materials ScienceOrthorhombic crystal systemGrain boundaryCeramicInstrumentationElectrical impedancePhase Transitions
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Polar phonons in relaxor ferroelectric 0.2PSN-0.4PMN-0.4PZN

2008

Relaxor ferroelectrics 0-2PbSc(1/2)Nb(1/2)O(3) - 0.4PbMg(1/3)Nb(2/3)O(3)-0.4PbZn(1/3)Nb(2/3)O(3) ceramics were studied by means of the Fourier transform infrared reflection and THz transmission spectroscopy in the temperature range of 20-500 K. On heating from low temperatures, the A(1) component of the strongly split TO1 mode softens towards the Burns temperature, but the softening ceases near 400 K, which could be a signature of polar cluster percolation temperature.

Materials scienceCondensed matter physicsPhononInfraredGeneral Physics and AstronomyAtmospheric temperature rangesymbols.namesakeFourier transformReflection (mathematics)visual_artPercolationsymbolsvisual_art.visual_art_mediumCeramicBurns temperature
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Far-infrared and THz spectroscopy of 0.4PMN–0.3PSN–0.3PZN relaxor ferroelectric ceramics

2007

Abstract Temperature dependence of the optic phonons in 0.4PbMg 1/3 Nb 2/3 O 3 –0.3PbSc 1/2 Nb 1/2 O 3 –0.3PbZn 1/3 Nb 2/3 O 3 (0.4PMN–0.3PSN–0.3PZN) ceramics were studied by means of FTIR reflection and THz transmission spectroscopy in the temperature range of −253.15 to 226.85 °C. On heating from low temperatures, the A 1 component of the strongly split TO 1 mode softens towards the Burns temperature, but the softening ceases near 126.85 °C which could be a signature of polar cluster percolation temperature. Surprisingly, the TO 2 mode also softens on heating and follows the Cochran law with extrapolated critical temperature close to the melting point.

Materials scienceCondensed matter physicsPhononMineralogyAtmospheric temperature rangeFar infraredvisual_artPercolationMaterials ChemistryCeramics and CompositesMelting pointvisual_art.visual_art_mediumCeramicSpectroscopyBurns temperatureJournal of the European Ceramic Society
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Soft mode in PMN–PSN ceramics

2008

Various ordered and disordered (1–x)Pb(Mg1/3Nb2/3)O3 –x Pb(Sc1/2Nb1/2)O3 (PMN–PSN) ceramics were studied by THz transmission spectroscopy in the temperature range of 10–300 K. It is found that the dielectric relaxation dominates in the spectra in higher temperatures, T > 170 K. In contrast, below 150 K, the strength of relaxation becomes so weak that the phonon contribution can be separated. The phonon contributribution in the investigated frequency range (200 GHz–2 THz) is presumably caused by the E component of the Last mode. The component exhibits hardening on cooling in all investigated ceramics and its critical temperature in ferroelectric PMN–PSN ceramics (x = 1, 0.95) is lower than t…

Materials scienceCondensed matter physicsPhononMineralogyDielectricSoft modesAtmospheric temperature rangeCondensed Matter PhysicsFerroelectricitySpectral lineElectronic Optical and Magnetic Materialsvisual_artvisual_art.visual_art_mediumHardening (metallurgy)Ceramicphysica status solidi (b)
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Bright Beaches of Nanoscale Potassium Islands on Graphite in STM Imaging

2008

We demonstrate, via scanning tunneling microscopy (STM) measurements performed at 48 K, the existence of "bright beaches" at the edges of K islands (diameter approximately 5-500 nm) on the graphite surface. The enhanced tunneling current is only observed in monolayer-high islands on graphite, and not in islands of similar geometry on top of a K monolayer film. First-principles density functional calculations and STM simulations suggest that this is an STM field effect, which appears as the positive tip attracts donated electrons back to the metallic K islands. The restored charge accumulates preferentially at the island edges.

Materials scienceCondensed matter physicsPotassiumGeneral Physics and Astronomychemistry.chemical_elementField effectNanotechnologyElectronlaw.inventionMetalchemistrylawvisual_artMonolayervisual_art.visual_art_mediumGraphiteScanning tunneling microscopeNanoscopic scalePhysical Review Letters
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Broad Distribution of Relaxation Times in 0.6PMN-0.4PZN Relaxor Ceramics

2007

In this paper dielectric spectra of 0.6PMN-0.4PZN ceramic obtained from broadband dielectric spectroscopy is presented. Measurements revealed an unusual relaxor like nature. Two different processes in the dielectric spectra have been observed. High frequency, or short relaxation times, behaviour is typical for ferroelectric crystals. Longest relaxation times do not follow Vogel—Fulcher dependence, which is unusual for relaxors.

Materials scienceCondensed matter physicsRelaxation (NMR)Condensed Matter PhysicsFerroelectricityZirconateElectronic Optical and Magnetic MaterialsDielectric spectroscopyDistribution (mathematics)Nuclear magnetic resonancevisual_artvisual_art.visual_art_mediumCeramicCole–Cole equationBroadband dielectric spectroscopyFerroelectrics
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Chemical strain effects and changed lattice dynamic in (Sr1-1.5xBix)TiO3ceramics (x ≤ 0.15)

2016

ABSTRACTIn this work lattice strain (induced by chemical Bi substitution on A-site) effects on the lattice dynamic of SrTiO3 ceramics were investigated by broadband dielectric spectroscopy in the very broad frequency range from 10 mHz up to 30 GHz and temperatures from 30 K to 500 K. Obtained results confirmed predicted induce of the ferroelectricity and suppression of the structural phase transition due to substitution of A-site ions – chemical straining of the lattice, both happening at the local scale but evident in macroscopic dielectric spectroscopy measurements. Calculated relaxation time distribution function broadens towards the longest relaxation times with temperature decrease and…

Materials scienceCondensed matter physicsRelaxation (NMR)Doping02 engineering and technology021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesFerroelectricityElectronic Optical and Magnetic MaterialsDielectric spectroscopyIonCondensed Matter::Materials ScienceDistribution functionNuclear magnetic resonanceLattice (order)visual_art0103 physical sciencesvisual_art.visual_art_mediumCeramic010306 general physics0210 nano-technologyFerroelectrics
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Dielectric relaxation in crystals and ceramics derived from BaTiO3

1992

Abstract A dielectric relaxation is reported in a crystal of BaTiO3 and in ceramics with composition (Ba1-yCay)TiO3 (0≤y≤0.2) in the frequency and temperature ranges 106 to 109 Hz and 350 to 450 K, respectively. A minimum of the relaxation frequency occurs close to the ferroelectric Curie temperature. The relaxation is of dipolar-type.

Materials scienceCondensed matter physicsRelaxation frequencyDielectricCondensed Matter PhysicsFerroelectricityElectronic Optical and Magnetic MaterialsCrystalvisual_artvisual_art.visual_art_mediumRelaxation (physics)Curie temperatureCeramicCole–Cole equationFerroelectrics
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Electrical Transport Properties of Lead−Free (Na0.5Bi0.5)1-xBaxZr0.04Ti0.96O3Ceramics (x = 0.06, 0.085, 0.1)

2011

Lead-free ceramics (Na0.5Bi0.5)1-xBaxZr0.04Ti0.96O3 were prepared by solid phase hot pressing sintering process. Density values of obtained samples are higher than 95% of the theoretical ones. Samples with x = 0.06, 0.085 and 0.1 were investigated in the present work. For these samples both ac and dc electric conductivity were studied. A low frequency (100 Hz-100 kHz) ac conductivity obeys the power law, characteristic for disordered materials. The dc conductivity has a thermally activated character. A barrier hopping model is found to explain the mechanism of charge transport in these materials. The (Na0.5Bi0.5)1-xBaxZr0.04Ti0.96O3 system is expected to be a new and promising candidate for…

Materials scienceCondensed matter physicsSinteringLow frequencyCondensed Matter PhysicsHot pressingFerroelectricityPower lawElectronic Optical and Magnetic MaterialsElectrical resistivity and conductivityvisual_artPhase (matter)visual_art.visual_art_mediumCeramicFerroelectrics
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Dielectric spectra of electron-irradiated PSN ceramics

1997

The influence of electron-irradiation on the dielectric properties of transparent PSN ferroelectric ceramics is studied by low (LF) and infralow (ILF) frequency spectrum analysis. Redistribution of relaxation frequencies caused by electron-irradiation has been discovered and is related to pinning impacts of the radiation-induced defects.

Materials scienceCondensed matter physicsSolid-state physicsFerroelectric ceramicschemistry.chemical_elementDielectricElectronElectroluminescenceThuliumNuclear magnetic resonancechemistryvisual_artvisual_art.visual_art_mediumIrradiationCeramicSPIE Proceedings
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