Search results for "Surfaces"

showing 10 items of 2837 documents

First principles simulations of 2D Cu superlattices on the MgO(0 0 1) surface

2004

AbstractFirst principles slab simulations of copper 2D superlattices of different densities on the perfect MgO(001) surface are performed using the DFT method as implemented into the CRYSTAL98 computer code. In order to clarify the nature of interfacial bonding, we consider regular 1/4, 1/2 and 1 monolayer (ML) coverages and compare results of our calculations with various experimental and theoretical data. Our general conclusion is that the physical adhesion associated with a Cu polarization and charge redistribution gives the predominant contribution to the bonding of the regular Cu 2D layer on the MgO(001) surface.

Condensed matter physicsChemistrySuperlatticeAb initioGeneral Physics and Astronomychemistry.chemical_elementSurfaces and InterfacesGeneral ChemistryCondensed Matter PhysicsAtomic unitsCopperMgO(001) surfaceSurfaces Coatings and FilmsCrystallographyTransition metalAb initio quantum chemistry methodsMonolayerSlabAb initio calculationsSuperlatticeCuCopper adhesionApplied Surface Science
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Calculations of the atomic and electronic structure for SrTiO3 perovskite thin films

2001

The results of calculations of SrTiO3 (100) surface relaxation and rumpling with two different terminations (SrO and TiO2) are presented and discussed. We have used the ab initio Hartree–Fock (HF) method with electron correlation corrections and the density functional theory (DFT) with different exchange–correlation functionals, including hybrid exchange techniques. All methods agree well on surface energies and on atomic displacements, as well as on the considerable increase of covalency effects near the surface. More detailed experiments on surface rumpling and relaxation are necessary for further testing of theoretical predictions.

Condensed matter physicsElectronic correlationChemistryMetals and AlloysAb initioSurfaces and InterfacesElectronic structureMolecular physicsSurface energySurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceAb initio quantum chemistry methodsPhysics::Atomic and Molecular ClustersMaterials ChemistryRelaxation (physics)Density functional theoryLocal-density approximationThin Solid Films
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Thickness scaling of space-charge-limited currents in organic layers with field- or density-dependent mobility

2006

An exact solution is provided for the current density-voltage (J –V) characteristics of space-charge limited transport of a single carrier in organic layers with field-dependent mobility of the type μ (E) = μ0 exp (γ √E. The general scaling relationship for field-dependent mobility occurs in terms of the variables JL and V /L. For the density-dependence of the mobility found in organic field-effect transistor measurements, the thickness scaling occurs in terms of different variables, J1/βL and V /L. The proposed scaling is a useful test for distinguishing field- and carrier density-dependent mobility in disordered organic semiconductors. (© 2006 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

Condensed matter physicsField (physics)ChemistryTransistorSurfaces and InterfacesCondensed Matter PhysicsSpace chargeSurfaces Coatings and FilmsElectronic Optical and Magnetic Materialslaw.inventionOrganic semiconductorExact solutions in general relativitylawDensity dependentMaterials ChemistryElectrical and Electronic EngineeringScalingphysica status solidi (a)
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Domain wall splitting and creation of the fine domain structure

1998

Abstract The study of the movement of the paraelectric-ferroelectric interphase boundary in (Ba,Sr)TiO 3 with concentration change is provided in the framework of the mean-field theory. The analytical solution for the parameters of motion of the interphase boundary is applied to the calculations of the splitting of domain walls in (Ba,Sr)TiO 3 for different concentrations of Sr. The calculations are based on the experimental data for the Curie–Weiss constant and for the parameters of the Landau–Ginzburg expression for the free energy.

Condensed matter physicsMetals and AlloysBoundary (topology)Surfaces and InterfacesSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials Sciencechemistry.chemical_compoundDomain wall (magnetism)Mean field theorychemistryDomain (ring theory)Materials ChemistryStrontium titanateInterphaseConstant (mathematics)Solid solutionThin Solid Films
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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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Pressure Effect on Spin Crossover in [Fe(phen)2(NCS)2] and [CrI2(depe)2]

2004

In the present article, we discuss the results of investigations of the influence of hydrostatic pressure (up to 1.2 GPa) on the spin transition behavior in [Fe(phen)2(NCS)2] polymorph II and [CrI2(depe)2]. It is demonstrated that pressure effect studies are very helpful in elucidating the mechanism of cooperative dynamic electronic structure phenomena accompanied by significant volume changes. Application of hydrostatic pressure serves as a tool for modifying the ligand field strength in a controlled manner.

Condensed matter physicsSpin crossoverChemistryHydrostatic pressureSpectrochemical seriesMaterials ChemistrySpin transitionPhysical chemistryElectronic structurePhysical and Theoretical ChemistrySurfaces Coatings and FilmsThe Journal of Physical Chemistry B
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Lattice gas models for multilayer adsorption: variation of phase diagrams with the strength of the substrate potential

1990

Abstract The simple cubic lattice gas model with nearest-neighbor attractive interaction is considered for the case where the potential V ( z ), that an adatom at a distance z from the surface experiences due to the substrate, is V ( z ) = − A / z 3 . Exact ground state phase diagrams are obtained for different A , while the behavior at nonzero temperatures is studied both by Monte Carlo simulations and the molecular field approximation. We show that the detailed sequence of the layering transitions in the first few layers depends very strongly on the strength of the substrate potential: for strong potentials individual first-order layering transitions in layers 1, 2, 3, …, while for interm…

Condensed matter physicsTriple pointChemistryMonte Carlo methodThermodynamicsSimple cubic latticeSurfaces and InterfacesCondensed Matter PhysicsSurfaces Coatings and FilmsAdsorptionLattice (order)Materials ChemistryLayeringGround statePhase diagramSurface Science
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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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Coulomb blockade nanothermometer

1998

Reliable thermometry is normally based on commercial secondary sensors which are factory calibrated. Primary thermometers exist, too, but their use is limited because of intrinsic slowness, complex instrumentation, or inconvenient installation at the desired location. We have found that arrays of nanoscale tunnel junctions exhibit properties which are very suitable for primary and secondary cryogenic thermometry. Temperature range of this Coulomb blockade thermometer (CBT) extends over about two decades for one sensor and the mean temperature is lithographically adjustable. We have studied the performance of the CBT sensors at very low temperatures where the minimum temperature is limited b…

Condensed matter physicsbusiness.industryChemistryInstrumentationCoulomb blockadeElectronRadiationAtmospheric temperature rangeCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsAtomic and Molecular Physics and OpticsSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsMagnetic fieldTunnel junctionThermometerOptoelectronicsElectrical and Electronic EngineeringbusinessMicroelectronic Engineering
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Comparative study of [001] surface relaxations of perovskite titanates

1998

Surface relaxations of the cubic perovskite SrTiO and BaTiO crystals have been studied in the framework of the shell model. The 33 positions of atoms in several surface layers embedded into the electrostatic field of the remainder of the crystal were calculated. Ti 4q , Sr 2q ,B a 2q and O 2y ions in six near-surface layers are displaced differently from their crystalline sites. Such effects create the so-called surface rumpling, a dipole moment and the electric field in the near-surface region. Calculated atomic displacements were compared with the LEED experimental data and showed good agreement. Our simulations have demonstrated that the cubic perovskite SrTiO crystals 3 reveal surface p…

Condensed matter physicsbusiness.industryRelaxation (NMR)Metals and AlloysSurfaces and InterfacesDielectricFerroelectricitySurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsCrystalDipolechemistry.chemical_compoundOpticschemistryElectric fieldMaterials ChemistryStrontium titanatebusinessPerovskite (structure)Thin Solid Films
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