Search results for "Crystal system"

showing 10 items of 13557 documents

First-principles calculations on double-walled inorganic nanotubes with hexagonal chiralities

2011

The two sets of commensurate double-walled boron nitride and titania hexagonally-structured nanotubes (DW BN and TiO2 NTs) possessing either armchair- or zigzag-type chiralities have been considered, i.e., (n1,n1)@(n2,n2) or (n1,0)@(n2,0), respectively. For symmetry analysis of these nanotubes, the line symmetry groups for one-periodic (1D) nanostructures with rotohelical symmetry have been applied. To analyze the structural and electronic properties of hexagonal DW NTs, a series of large-scale ab initio DFT-LCAO calculations have been performed using the hybrid Hartree-Fock/Kohn-Sham exchange-correlation functional PBE0 (as implemented in CRYSTAL-09 code). To establish the optimal inter-sh…

Condensed Matter::Materials Sciencechemistry.chemical_compoundReflection symmetryNanostructureDouble walledCondensed matter physicsChemistryBoron nitrideHexagonal crystal systemPhysics::Atomic and Molecular ClustersAb initioTotal energySymmetry (physics)IOP Conference Series: Materials Science and Engineering
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Variation of the optical absorption edge in AgGaS2 single crystals at high pressure

2003

In this paper the optical absorption edge of AgGaS 2 is measured as a function of pressure up to 26 GPa in order to verify the effect of the three phases transitions occurring in that pressure domain. The direct energy gap increases linearly with pressure at the rate of about 4.0 x 10 -2 eV GPa -1 up to 10.2 GPa. The absence of any discontinuity in the energy gap in the pressure range of 4.2-10.2 GPa confirms that the volume change, in the chalcopirite to monoclinic second-order transition, if it exists, is very small. When the pressure is raised above 10.2 GPa, the energy gap drops suddenly by about 1.1 eV and the spectral form of the absorption coefficient is typical of semiconductors wit…

Condensed matter physicsAbsorption spectroscopybusiness.industryAnnealing (metallurgy)Band gapChemistryCondensed Matter PhysicsPressure coefficientElectronic Optical and Magnetic MaterialsSemiconductorOpticsAbsorption edgeAttenuation coefficientbusinessMonoclinic crystal systemphysica status solidi (b)
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Magnetic exchange interaction in a pair of orbitally degenerate ions: Magnetic anisotropy of [Ti2Cl9]−3

2001

The theory of the kinetic exchange in a pair of orbitally degenerate ions developed by the authors [J. Phys. Chem. A 102, 200 (1998)] is applied to the case of face-shared bioctahedral dimer (overall D3h-symmetry). The effective kinetic exchange Hamiltonian is found for a 2T2–2T2 system taking into account all relevant transfer pathways and charge-transfer crystal field states. The influence of different transfer integrals involved in the kinetic exchange on the energy pattern and magnetic properties of the system is examined. The role of other related interactions (trigonal crystal field, spin–orbit coupling) is also discussed in detail. Using the pseudoangular momentum representation and …

Condensed matter physicsChemistryDegenerate energy levelsGeneral Physics and AstronomyTrigonal crystal systemKinetic energyNegative ionsExchange interactions (electron)Magnetic exchangeIonUNESCO::FÍSICA::Química físicaMagnetic anisotropysymbols.namesakeTitanium compounds ; Magnetic anisotropy ; Negative ions ; Exchange interactions (electron)Quantum mechanicssymbolsTitanium compoundsPhysical and Theoretical Chemistry:FÍSICA::Química física [UNESCO]Hamiltonian (quantum mechanics)Magnetic anisotropy
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Orbitally dependent kinetic exchange in cobalt(II) pairs: origin of the magnetic anisotropy

2003

Abstract A comprehensive theoretical study of the magnetic exchange between Co 2+ ions is reported. Using the microscopic background we deduce the general Hamiltonian for a corner-shared bioctahedral system involving kinetic exchange, spin–orbit coupling and low-symmetry local crystal field. This Hamiltonian acting within orbitally degenerate ground manifold 4 ( T 1g ) A ⊗ 4 ( T 1g ) B of the cobalt pair is expressed in terms of orbital and spin operators. We elucidate the major electronic factors controlling the exchange anisotropy in the Co(II) pairs. The degree of the magnetic anisotropy is shown to depend on the strength of the cubic crystal field and on the relative efficiency of two k…

Condensed matter physicsChemistryDegenerate energy levelsSpin–orbit interactionCubic crystal systemInorganic ChemistryMagnetic anisotropysymbols.namesakeExchange biasMagnetochemistryMaterials ChemistrysymbolsPhysical and Theoretical ChemistryAnisotropyHamiltonian (quantum mechanics)Polyhedron
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Anomalies in low-temperature lattice parameters of ErFeO3 and ErAlO3 single crystals: correlation with magnetic properties

2005

Abstract The paper presents the results of an experimental study of thermal expansion of isostructural orthorhombic ErFeO3 and ErAlO3 single crystals. Changes of lattice parameters have been investigated by X-ray measurements in the 10–300 K temperature range. Above ∼150 K, experimental results correspond well to the phonon mechanism. At low temperatures distinct anisotropic anomalies were observed in both compounds; and a correlation with the magnetic properties of the relevant ions is noted.

Condensed matter physicsChemistryPhononGeneral ChemistryAtmospheric temperature rangeCondensed Matter PhysicsThermal expansionIonCondensed Matter::SuperconductivityLattice (order)Materials ChemistryCondensed Matter::Strongly Correlated ElectronsOrthorhombic crystal systemIsostructuralAnisotropySolid State Communications
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Incommensurate phases in adsorbed monolayers: structure and energy of domain walls

2002

Abstract The properties of incommensurate films of domain-wall structure formed on the (1 0 0) plane of face centered cubic crystals are studied by Monte Carlo simulation. The wall energies, wall structure and the wall–wall interaction are determined for different types of domain walls occurring in films which form the c(2×2) registered structure. The systems characterized by different strength and corrugation of the surface potential and of different misfit between adsorbate and adsorbent are discussed. It is demonstrated that heavy as well as light walls are rather strongly localized. Moreover, it is shown that the incommensurate structure with crossing heavy walls has higher stability th…

Condensed matter physicsChemistryPlane (geometry)Monte Carlo methodSurfaces and InterfacesCubic crystal systemCondensed Matter PhysicsEpitaxySurfaces Coatings and FilmsPhysics::Fluid DynamicsAdsorptionPhysisorptionPhase (matter)MonolayerMaterials ChemistrySurface Science
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Vibrational properties of ZnTe at high pressures

2002

Raman spectra of ZnTe were measured under hydrostatic pressures up to 15 GPa at T = 300 K. Results for the frequencies of first- and second-order Raman features of the zincblende phase (0-9.5 GPa) are used to set up a rigid-ion model of the phonon dispersion relations under pressure. Calculated phonon densities of states, mode Gruneisen parameters and the thermal expansion coefficient as a function of pressure are discussed. The effect of pressure on the widths and intensities of Raman spectral features is considered. Raman spectra of high-pressure phases of ZnTe are reported. These spectra indicate the possible existence of a new phase near 13 GPa, intermediate between the cinnabar and ort…

Condensed matter physicsPhononChemistryHydrostatic pressureCondensed Matter PhysicsThermal expansionCondensed Matter::Materials Sciencesymbols.namesakeCondensed Matter::SuperconductivityMolecular vibrationDispersion relationPhase (matter)symbolsGeneral Materials ScienceOrthorhombic crystal systemRaman spectroscopyJournal of Physics: Condensed Matter
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Monte Carlo Study of Dense Monolayer and Bilayer Films on the (100) Plane of Face-Centered Cubic Crystals

1999

A Monte Carlo simulation method in the canonical and in the grand canonical ensembles is used to study the behavior and properties of dense monolayer and bilayer films formed on the (100) plane of model face-centered cubic crystals. Systems with different effects due to the periodicity of the gas−solid potential are considered, and the mechanism of melting in the first and the second adsorbed layer is discussed. It is demonstrated that the film structure is very sensitive to the gas−solid potential corrugation, as well as to the temperature and the surface coverage. In particular, it is shown that monolayer films formed on weakly corrugated surfaces exhibit the incommensurate (dense) phase …

Condensed matter physicsPlane (geometry)ChemistryBilayerTransition temperatureMonte Carlo methodSurfaces and InterfacesCubic crystal systemCondensed Matter PhysicsPhase (matter)MonolayerElectrochemistryGeneral Materials ScienceSpectroscopyPhase diagramLangmuir
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Spin crossover behaviour in the iron(II)-2,2-dipyridilamine system: Synthesis, X-ray structure and magnetic studies

2005

Abstract The monomeric compounds [Fe(dpa)2(X)2] · solv [X = NCS−(solv = 0.5H2O) (1), N ( CN ) 2 - (2) and dpa = 2,2-dipyridilamine] have been synthesised and characterised. They crystallise in the P21/n and in the Cc monoclinic systems, respectively. Four of six nitrogen atoms coordinated to the Fe(II) ions belong to two dpa ligands which lie in cis conformation. The remaining positions are occupied by two nitrogen atoms of the pseudo-halide ligands. The magnetic susceptibility measurements at ambient pressure have revealed that compound 1 exhibits an incomplete spin crossover behaviour (T1/2 ≈ 88 K), whereas compound 2 remains in the high-spin configuration. Pressure studies performed on c…

Condensed matter physicsX-raychemistry.chemical_elementNitrogenMagnetic susceptibilityIonInorganic Chemistrychemistry.chemical_compoundCrystallographyMonomerchemistrySpin crossoverMaterials ChemistryPhysical and Theoretical ChemistryMonoclinic crystal systemAmbient pressureInorganica Chimica Acta
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Semiconducting half-Heusler and LiGaGe structure type compounds

2009

Compounds with LiAlSi (half-Heusler) and LiGaGe structure types have been investigated by means of band structure calculations. The LiAlSi structure type is known as the half-Heusler structure type, whereas LiGaGe is a closely related hexagonal variant. A remarkable feature of some XYZ half-Heusler compounds with 8 and 18 valence electrons is, that despite being composed of only metallic elements, they are semiconductors. More than 100 semiconducting compounds within these structure types are known. LiGaGe compounds have an additional degree of freedom, namely the degree of puckering of the layers. These compounds can become semiconducting at a certain degree of puckering. Half-metallic beh…

Condensed matter physicsbusiness.industryChemistryHexagonal crystal systemSurfaces and InterfacesStructure typeElectronic density of statesCondensed Matter PhysicsSemimetalSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsMetalSemiconductorvisual_artMaterials Chemistryvisual_art.visual_art_mediumElectrical and Electronic EngineeringbusinessValence electronElectronic band structurephysica status solidi (a)
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