Search results for "Surfaces"

showing 10 items of 2837 documents

Ab initio modeling of copper adhesion on regular BaTiO3(001) surfaces

2005

Ab initio calculations have been performed for copper adsorption on a regular, defect-free TiO"2- and BaO-terminated (001) surfaces of a cubic BaTiO"3, using a posteriori HF-CC method as implemented into the CRYSTAL-03 computer code. To clarify the nature of the interfacial bonding, we use slab models of the Cu/BaTiO"3(001) interfaces with different one-side substrate coverages, varied from 1/8 monolayer (ML) up to 1/2 ML, over both TiO"2- and BaO-terminated surfaces. TiO"2 termination has been found to be energetically more favorable for the adsorption of copper atoms. In agreement with previous experimental and theoretical data, our calculations indicate essential contribution of atomic p…

ChemistryBinding energyAb initiochemistry.chemical_elementSubstrate (electronics)Electronic structureCondensed Matter PhysicsCopperAtomic and Molecular Physics and OpticsSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsAdsorptionAb initio quantum chemistry methodsChemical physicsMonolayerElectrical and Electronic EngineeringAtomic physicsMicroelectronic Engineering
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Transport equations of electrodiffusion processes in the laboratory reference frame.

2006

The transport equations of electrodiffusion processes use three reference frames for defining the fluxes: Fick's reference in diffusion, solvent-fixed reference in transference numbers, and laboratory fluxes in electric conductivity. The convenience of using only one reference frame is analyzed here from the point of view of the thermodynamics of irreversible processes. A relation between the fluxes of ions and solvent and the electric current density is deduced first from a mass and volume balance. This is then used to show that (i) the laboratory and Fick's diffusion coefficients are identical and (ii) the transference numbers of both the solvent and the ion in the laboratory reference fr…

ChemistryBoundary (topology)ThermodynamicsMechanicsSurfaces Coatings and FilmsIonElectrical resistivity and conductivityMaterials ChemistryPhysical and Theoretical ChemistryElectric currentExperimental methodsDiffusion (business)Volume balanceReference frameThe journal of physical chemistry. B
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Capillary Hysteresis in Nanopores: Theoretical and Experimental Studies of Nitrogen Adsorption on MCM-41

1995

Capillary hysteresis in cylindrical nanopores has been studied using MCM-41 as the prime example of a mesoporous material. These materials, due to their regular pore structure, can be considered to be candidates for reference adsorbents for standardizing adsorption measurements and methods for characterization of porous solids. They provide a unique opportunity for verification of theoretical models employed for predicting phase equilibrium in confined geometry. Three samples with monodisperse pore channels have been synthesized and examined using X-ray diffraction (XRD). Nitrogen adsorption isotherms were modeled using nonlocal density functional theory (NLDFT) in a wide range of pore size…

ChemistryCapillary actionDispersityMineralogyThermodynamicsSurfaces and InterfacesCondensed Matter PhysicsCondensed Matter::Materials ScienceNanoporeHysteresisAdsorptionMetastabilityElectrochemistryGeneral Materials ScienceDensity functional theoryMesoporous materialSpectroscopyLangmuir
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A vacuum cell for obtaining clean surfaces on liquid low melting point metals

1997

Abstract Clean oxide film-free surface of liquid gallium was obtained in a sealed vacuum cell with a glass lid for observation. The cell was evacuated to high vacuum (10 -4 Pa) before admission of liquid and sealing. The surface contamination was about 2–5% of the free area and did not exhibit noticeable increase during several months of storing and employing the cell. The cell described allows observation of surface flows, capillary phenomena and crystallization processes under different conditions.

ChemistryCapillary actionbusiness.industryUltra-high vacuumOxideLow melting pointContaminationCondensed Matter PhysicsSurfaces Coatings and Filmslaw.inventionchemistry.chemical_compoundOpticsChemical engineeringlawCrystallizationLiquid galliumbusinessInstrumentationVacuum
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Full configuration interaction calculation of BeH adiabatic states.

2008

An all-electron full configuration interaction (FCI) calculation of the adiabatic potential energy curves of some of the lower states of BeH molecule is presented. A moderately large ANO basis set of atomic natural orbitals (ANO) augmented with Rydberg functions has been used in order to describe the valence and Rydberg states and their interactions. The Rydberg set of ANOs has been placed on the Be at all bond distances. So, the basis set can be described as 4s3p2d1f3s2p1d(BeH)+4s4p2d(Be). The dipole moments of several states and transition dipole strengths from the ground state are also reported as a function of the R(Be-H) distance. The position and the number of states involved in sever…

ChemistryConfiguration interactionsGeneral Physics and AstronomyBond lengthsBeryllium compounds ; Bond lengths ; Configuration interactions ; Ground states ; Molecular moments ; Potential energy surfaces ; Rydberg states ; Vibrational statesRydberg statesPotential energyFull configuration interactionGround statesUNESCO::FÍSICA::Química físicaDipolesymbols.namesakeAtomic orbitalBeryllium compoundsPotential energy surfacesRydberg formulasymbolsMolecular momentsVibrational statesPhysical and Theoretical ChemistryAtomic physicsGround stateAdiabatic process:FÍSICA::Química física [UNESCO]Basis setThe Journal of chemical physics
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On the relaxation mechanisms of 6-azauracil

2011

The nonadiabatic photochemistry of 6-azauracil has been studied by means of the CASPT2//CASSCF protocol and double-ζ plus polarization ANO basis sets. Minimum energy states, transition states, minimum energy paths, and surface intersections have been computed in order to obtain an accurate description of several potential energy hypersurfaces. It is concluded that, after absorption of ultraviolet radiation (248 nm), two main relaxation mechanisms may occur, via which the lowest (3)(ππ*) state can be populated. The first one takes place via a conical intersection involving the bright (1)(ππ*) and the lowest (1)(nπ*) states, ((1)ππ*/(1)nπ*)(CI), from which a low-energy singlet-triplet crossin…

ChemistryConical intersectionPotential energyTransition stateSurfaces Coatings and FilmsMaterials ChemistryEnergy levelQuantum TheoryThermodynamicsPhysical and Theoretical ChemistryAtomic physicsTriplet stateGround stateUracilUltraviolet radiationFOTOQUÍMICA
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Dopamine interaction with a polyamine cryptand of 1H-pyrazole in the absence and in the presence of Cu(ii) ions. Crystal structure of [Cu2(H−1L](ClO4…

2000

The crystal structure of the binuclear Cu2+ complex [Cu2(H−1L)](ClO4)3 ·2H2O of the cryptand L = 1,4,7,8,11,14,17,20,21,24,29,32,33,36-tetradecaazapentacyclo[12.12.12.1 6,9.119,22,1,31,34]hentetraconta-6,9(41), 19(40), 21,31,34(39)-hexaene is presented; evidence for the formation in solution of binary L–dopamine and ternary Cu2+–L–dopamine complexes is presented.

ChemistryCryptandMetals and AlloysGeneral ChemistryCrystal structurePyrazoleCatalysisSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsIonCrystallographychemistry.chemical_compoundDopamineMaterials ChemistryCeramics and CompositesmedicineTernary operationPolyaminemedicine.drugChemical Communications
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A Density Functional Theory study on gold cyanide interactions: The fundamentals of ore cleaning

2010

We have employed Density Functional Theory calculations to study the adsorption of CN, CN− and KCN on Au(111) and Au(211) surfaces and compare the obtained results to CO. The adsorption of CN, CN−, and KCN are exothermic with respect to the gas-phase moieties, and the adsorption energy increases at steps. Our results show that the binding mechanism of CN− is different from that of CO. The projected LDOS indicates that the bond between the flat surface and CN shows very small overlap between metal and CN states. This overlap increases provided that extra charge is present or low-coordinated Au atoms are available. Charge transfer is analyzed via the Bader method and the Electron Localization…

ChemistryCyanideInorganic chemistrySurfaces and InterfacesCondensed Matter PhysicsElectron localization functionSurfaces Coatings and FilmsMetalchemistry.chemical_compoundElectron transferAdsorptionTransition metalCovalent bondvisual_artMaterials Chemistryvisual_art.visual_art_mediumPhysical chemistryDensity functional theorySurface Science
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Analysis and parametric sensitivity of the behavior of overshoots in the concentration of a charged adsorbate in the adsorbed phase of charged adsorb…

2003

In this work, an analysis of the parametric sensitivity of the overshoot in the concentration of the adsorbate in the adsorbed phase, which occurs under certain conditions during an ion-exchange adsorption process, is presented and used to suggest practical implications of the concentration overshoot phenomenon on operational policies and configurations of chromatographic columns and finite bath adsorption systems. The results presented in this work demonstrate and explain how the development of an overshoot in the concentration of the adsorbate in the adsorbed phase could be enhanced or suppressed by (i) varying the diffusion coefficient, D3, of the adsorbate relative to the diffusion coef…

ChemistryDiffusionAnalytical chemistryLangmuir adsorption modelThermodynamicsElectrolyteCharged particleSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsBiomaterialssymbols.namesakeColloid and Surface ChemistryAdsorptionIonic strengthPhase (matter)symbolsDebye lengthJournal of Colloid and Interface Science
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Study of interface diffusion of Ti and TiN PVD layers by Bremsstrahlung-induced AES

1992

The influence of heat treatment in ultrahigh vacuum (UHV) on Ti and TiN layers coated by physical vapour deposition (PVD) has been studied by AES, XPS and bremsstrahlung-induced AES. It could be concluded that up to 500 o C (1 h) the Ti layer does not change significantly. At the TiN/steel substrate interface, however, a counter-diffusion of nitrogen and adventitious oxygen takes place, resulting in partial nitridation of the steel substrate and oxidation of the coating

ChemistryDiffusionAnalytical chemistrychemistry.chemical_elementSurfaces and InterfacesGeneral ChemistrySubstrate (electronics)engineering.materialCondensed Matter PhysicsOxygenNitrogenSurfaces Coatings and FilmsCoatingX-ray photoelectron spectroscopyChemical engineeringMaterials ChemistryengineeringTinLayer (electronics)Surface and Interface Analysis
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