Search results for "tetragonal crystal"

showing 10 items of 216 documents

High-pressure x-ray diffraction study of SrMoO4 and pressure-induced structural changes

2007

SrMoO4 was studied under compression up to 25 GPa by angle-dispersive x-ray diffraction. A phase transition was observed from the scheelite-structured ambient phase to a monoclinic fergusonite phase at 12.2(9) GPa with cell parameters a = 5.265(9) A, b = 11.191(9) A, c = 5.195 (5) A, and beta = 90.9, Z = 4 at 13.1 GPa. There is no significant volume collapse at the phase transition. No additional phase transitions were observed and on release of pressure the initial phase is recovered, implying that the observed structural modifications are reversible. The reported transition appeared to be a ferroelastic second-order transformation producing a structure that is a monoclinic distortion of t…

Condensed Matter - Materials SciencePhase transitionChemistrySpace groupMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesCrystal structureCondensed Matter PhysicsLandau theoryElectronic Optical and Magnetic MaterialsInorganic ChemistryTetragonal crystal systemCrystallographyPhase (matter)X-ray crystallographyMaterials ChemistryCeramics and CompositesPhysical and Theoretical ChemistryMonoclinic crystal system
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Iron-based Heusler compounds Fe2YZ: Comparison with theoretical predictions of the crystal structure and magnetic properties

2013

The present work reports on the new soft ferromagnetic Heusler phases Fe${}_{2}$NiGe, Fe${}_{2}$CuGa, and Fe${}_{2}$CuAl, which in previous theoretical studies have been predicted to exist in a tetragonal Heusler structure. Together with the known phases Fe${}_{2}$CoGe and Fe${}_{2}$NiGa these materials have been synthesized and characterized by powder x-ray diffraction, ${}^{57}$Fe M\"ossbauer spectroscopy, superconducting quantum interference device, and energy-dispersive x-ray measurements. In particular M\"ossbauer spectroscopy was used to monitor the degree of local atomic order/disorder and to estimate magnetic moments at the Fe sites from the hyperfine fields. It is shown that in con…

Condensed Matter::Materials ScienceTetragonal crystal systemMaterials scienceMagnetic momentFerromagnetismCondensed matter physicsAb initioCoherent potential approximationInverseElectronic structureCondensed Matter PhysicsHyperfine structureElectronic Optical and Magnetic MaterialsPhysical Review B
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Theoretical Prediction and Experimental Confirmation of Charge Transfer Vibronic Excitons and Their Phase in ABO3 Perovskite Crystals

2002

AbstractThe current theoretical and experimental knowledge of new polaronic-type excitons in ferroelectric oxides - charge transfer vibronic excitons (CTVE) is discussed. It is shown that quantum chemical Hartree-Fock-type calculations using a semiempirical Intermediate Neglect of Differential Overlap (INDO) method (modified for ionic/partly ionic solids) as well as photoluminescence studies in ferroelectric oxygen-octahedral perovskites confirm the CTVE existence. Our INDO calculations for KTaO3 and KNbO3 have demonstrated that the triplet exciton is a triad centre containing one active O atom and two Ta atoms sitting on the opposite sites from this O atom. The total energy of a system is …

Condensed Matter::Materials ScienceTetragonal crystal systemMaterials sciencePhotoluminescenceComputational chemistryExcitonAtomPhysics::Atomic and Molecular ClustersIonic bondingGround stateFerroelectricityMolecular physicsPerovskite (structure)MRS Proceedings
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Fine tuning of the magnetic properties in Mn3-Co Ga Heusler films near the critical regime

2021

Abstract Tunability of structural and magnetic properties of Mn3-xCoxGa films is presented by Co substitution, where critical behavior emerges 0.37 ≤ x ≤ 0.56 exhibiting a transition from tetragonal hard ferrimagnetic with perpendicular magnetic anisotropy (PMA) to a cubic soft ferrimagnetic phase with in-plane magnetic anisotropy (IMA). In the critical regime, coexisting state of tetragonal and cubic phases possesses significantly low coercive field (HC = 1.9 kOe) with relatively low saturation magnetization (MS = 100~150 emu/cc) while maintaining the PMA. From first-principles calculations, moments of two Mn sites do not change upon Co substitution. However, moments of substituted Co almo…

CouplingMaterials scienceCondensed matter physicsSpintronicsMechanical EngineeringMetals and Alloys02 engineering and technologyCoercivity010402 general chemistry021001 nanoscience & nanotechnologyAntiparallel (biochemistry)01 natural sciences0104 chemical sciencesTetragonal crystal systemMagnetic anisotropyMechanics of MaterialsFerrimagnetismPhase (matter)Materials Chemistry0210 nano-technologyJournal of Alloys and Compounds
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Structure and phase transitions in the ferroelastic [C(NH2)3]3Bi2Br9crystal

1999

Differential scanning calorimetry, dilatometric, dielectric and linear birefringence measurements have been used to study the ferroelastic [C(NH2)3]3Bi2Br9 crystal. The x-ray studies showed that it crystallizes at room temperature in the monoclinic symmetry, space group P21/m. The crystal undergoes a complex sequence of phase transitions: at 311 K, 333.5 K, 350 K, 415 K and 425 K. All phase transitions were found to be of first order type. The ferroelastic domain structure is maintained from room temperature up to 425 K. The temperature measurements of the linear birefringence and optical observations suggest the tetragonal symmetry of the parent paraelastic phase above 425 K.

CrystalPhase transitionCrystallographyTetragonal crystal systemDifferential scanning calorimetryBirefringenceChemistryPhase (matter)General Materials ScienceDielectricCrystal structureCondensed Matter PhysicsJournal of Physics: Condensed Matter
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Impurity levels and nonlinear optical properties of doped BaTiO3 from extended cluster LDA calculations

1997

The electronic structures of some transition-metal ions doping the ferroelectric oxide BaTiO3 are calculated through the density functional theory framework (LCAO-LSD ADF method) on extended clusters [XO6Ba8Ti6] embedded in a punctual charge set depicting the crystalline environment. The transition ions X are Fen+(n = 2, 3, 4, 5), Ti3+, Nb4+, and Nb5+. Some related defects like Fe(SINGLE BOND)Vo, where Vo stands for a lacunar oxygen site, are also investigated through a similar process. The positions of impurity levels insides the O2p(SINGLE BOND)Ti3d band gap are obtained from eigenvalues and related optical transition or ionization energies are calculated using excited states. This allows…

CrystalTetragonal crystal systemChemistryBand gapExcited stateSingle bondMolecular orbitalDensity functional theoryPhysical and Theoretical ChemistryIonization energyAtomic physicsCondensed Matter PhysicsAtomic and Molecular Physics and OpticsInternational Journal of Quantum Chemistry
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Crystal Field Excitations in CeAgl−xInx Compounds

1982

The substitution of the monovalent Ag for the trivalent In in LaAgl−xInx and CeAgl−xInx offers the possibility of influencing the conduction electron system in these compounds. The strong dependence of the spin susceptibility of La-systems on the In-concentration1 was interpreted by band calculations which suggest that the Fermi level is pushed into a region of a high 5d-eg-band density of states2. Furthermore, CeAgl−xInx is one of the rare 4f systems where a structural phase transition (from cubic to tetragonal) occurs prior to magnetic ordering. The ferromagnetic Curie temperature TC is roughly independent of x whereas the structural transition temperature Ts rises from 15 K for CeAg to a…

CrystalTetragonal crystal systemsymbols.namesakeMaterials scienceField (physics)FerromagnetismCondensed matter physicsFermi levelsymbolsCurie temperatureKnight shiftSpin (physics)
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Crystal structure and magnetism of the double perovskites A2FeReO6 (A=Ca, Sr, Ba)

2004

Abstract We synthesized a series of double perovskites A 2 FeReO 6 (A=Ca, Sr, Ba) with Curie temperatures above room-temperature. Neutron and X-ray diffraction analysis have been performed in order to determine the structural and (local) magnetic properties of these materials. While Ba 2 FeReO 6 stays cubic over the whole temperature range we examined, the Sr-compound shows a tetragonal distortion of the perovskite structure which does not completely vanish up to about 520 K far above T C . Ca 2 FeReO 6 has a monoclinic unit cell at high temperatures. Below 400 K a phase separation in two monoclinic phases with identical cell volume is observed in neutron scattering.

CrystallographyTetragonal crystal systemMaterials scienceCondensed matter physicsTransition temperatureNeutron diffractionCurie temperatureCrystal structureNeutron scatteringCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsPerovskite (structure)Monoclinic crystal systemJournal of Magnetism and Magnetic Materials
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The role of Nb in intensity increase of Er ion upconversion luminescence in zirconia

2014

It is found that Nb co-doping increases the luminescence and upconversion luminescence intensity in rare earth doped zirconia. Er and Yb-doped nanocrystalline samples with or without Nb co-doping were prepared by sol-gel method and thermally annealed to check for the impact of phase transition on luminescence properties. Phase composition and grain sizes were examined by X-ray diffraction; the morphology was checked by scanning- and high-resolution transmission electron microscopes. Both steady-state and time-resolved luminescence were studied. Comparison of samples with different oxygen vacancy concentrations and different Nb concentrations confirmed the known assumption that oxygen vacanc…

CrystallographyTetragonal crystal systemMaterials scienceNanocrystalDopingAnalytical chemistryGeneral Physics and AstronomyCubic zirconiaLuminescenceNanocrystalline materialPhoton upconversionIonJournal of Applied Physics
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Effect of cobalt doping on the dielectric response of $B_{0.95}Pb_{0.05}TiO_3$ ceramics

2013

Dielectric response of Ba 0.95 Pb 0.05 TiO 3 ceramics doped with 0.1 and 1 wt.% of Co 2 O 3 , synthesized by conven- tional high-temperature method, wa s studied in wide temperature and frequency range. The temperature dependences of the real and the imaginary parts of dielectric permittivity of the ceramics were compared with those of BaTiO 3 and Ba 0.95 Pb 0.05 TiO 3. The addition of Co 3+ ions results in a broadening of dielectric anom- alies related to the transition to p araelectric cubic phase, and the structural transition between the tetragonal and the orthorhombic phases. At low temperatures (125 – 200 K) the dielectric absorp- tion of Co-doped Ba 0.95 Pb 0.05 TiO 3 ceramics was fo…

Dielectric absorptionMaterials scienceCondensed matter physics$B_{0.95}Pb_{0.05}TiO_3$Dopingdeviation from the Curie-WeisslawDielectricCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsIonco-dopingTetragonal crystal systemDipoleMechanics of Materialsdielectric propertiesvisual_artMaterials ChemistryCeramics and Compositesvisual_art.visual_art_mediumOrthorhombic crystal systemCeramicElectrical and Electronic Engineering
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