Search results for "Ab initio quantum chemistry methods"

showing 10 items of 468 documents

Atomistic Simulations of the LaMnO3 (110) Polar Surface.

2003

The results of atomic structure calculations, with a focus on the surface relaxation and polarization, are presented for the LaMnO3 (110) O-terminated polar surface. We compare results of the classical shell model calculations for four possible terminations, including (1 × 2) (110) surface reconstruction, and demonstrate that the latter has the lowest surface energy. The surface energy is saturated only when six to eight near-surface atomic planes are relaxed which is accompanied by the considerable dipole moments perpendicular to the surface. Results are compared with those for iso-structural BaTiO3 (110) surfaces.

Surface (mathematics)ChemistrySHELL modelRelaxation (NMR)General Physics and AstronomyGeneral MedicinePolarization (waves)Molecular physicsSurface energyCrystallographyDipoleAb initio quantum chemistry methodsPerpendicularPolarPhysical and Theoretical ChemistrySurface reconstructionChemInform
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Ab Initio Calculations of Hydroxyl Impurities in CaF2

2012

OH– in CaF2 crystal and the (111) surface have been studied by using density functional theory (DFT) with hybrid exchange potentials, namely, DFT-B3PW. Three bulk and 20 surface OH– configurations ...

Surface (mathematics)CrystalGeneral EnergyChemistryComputational chemistryImpurityAb initio quantum chemistry methodsPhysical chemistryDensity functional theoryPhysical and Theoretical ChemistrySurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsThe Journal of Physical Chemistry C
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Ab Initio Calculations of SrTiO3 (111) Surfaces

2012

The paper presents the results of calculations of SrTiO3 polar (111) surface relaxations and energetics using the ab initio code CRYSTAL and a hybrid description of exchange and correlation. Using a hybrid B3LYP approach, the surface relaxation has been calculated for the two possible Ti and SrO3 SrTiO3 (111) surface terminations. For both Ti and SrO3-terminated SrTiO3 (111) surfaces upper layer atoms, with the sole exception of SrO3-terminated surface Sr atom, relax inwards. The calculated surface relaxation energy for Ti-terminated SrTiO3 (111) surface is almost five times larger, than the surface relaxation energy for SrO3-terminated SrTiO3 (111) surface. The surface energy for Ti-termin…

Surface (mathematics)CrystalMaterials scienceAb initio quantum chemistry methodsAtomAb initioRelaxation (physics)SIESTA (computer program)Molecular physicsSurface energy
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Theoretical Modelling of the Energy Surface (001) and Topology of CaZrO3 Perovskite

2015

I present the results of ab initio calculations of surface relaxations, rumplings, energetics, optical band gaps, and charge distribution for the CaZrO3 (001) surfaces using computer code CRYSTAL and a hybrid description of exchange and correlation. I consider both CaO and ZrO2-terminations of the CaZrO3 (001) surface. On the both CaO and ZrO2-terminated CaZrO3 (001) surfaces, I find that all upper and third layer atoms relax inwards, whereas all second layer atoms relax upwards. I predict a considerable increase of the Zr-O chemical bond covalency (0.102e) near the ZrO2-terminated CaZrO3 (001) surface relative to the CaZrO3 bulk (0.086e). My calculated CaO (0.87 eV) and ZrO2-terminated (1.…

Surface (mathematics)CrystalMaterials scienceChemical bondBand gapAb initio quantum chemistry methodsCharge densityAtomic physicsCondensed Matter PhysicsTopology (chemistry)Electronic Optical and Magnetic MaterialsPerovskite (structure)Ferroelectrics
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Ab initio Calculations of Bulk and (001) Surface F-centers in ABO3 Perovskites

2021

We analyzed systematic trends in BaTiO 3, SrTiO 3 , PbZrO 3 and SrZrO 3 bulk as well as very rarely performed (001) surface F-center ab initio calculations. The nearest neighbor atomic displacements around the bulk F-center in the ABO 3 perovskites are considerably smaller than the relevant neighbor atomic displacements around the (001) surface $F$ -centers. The $F$ -center electrons are more delocalized for the ABO 3 perovskite (001) surface $F$ -center than for the bulk $F$ -center. Our calculated formation energy differences between the BaTiO 3 , SrTiO 3 , PbZrO 3 and SrZrO 3 bulk and its (001) surface $F$ -centers triggers the $F$ -center segregation from the bulk crystal towards the AB…

Surface (mathematics)Delocalized electronMaterials scienceCondensed matter physicsAb initio quantum chemistry methodsElectronk-nearest neighbors algorithmPerovskite (structure)Bulk crystal2021 IEEE 12th International Conference on Electronics and Information Technologies (ELIT)
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Calculations of Surface Structure for SrTiO3 Perovskite

2001

ABSTRACTWe present and discuss results of the calculations for SrTiO3 (100) surface relaxation with different terminations (SrO and TiO2) using a semi-empirical shell model (SM) as well as abinitio methods based on Hartree-Fock (HF) and Density Functional Theory (DFT) formalisms. Using the SM, the positions of atoms in 16 near-surface layers placed atop a slab of rigid ions are optimized. This permits us determination of surface rumpling and surfaceinduced dipole moments (polarization) for different terminations. We also compare results of the ab initio calculations based on both HF with the DFT-type electroncorrelation corrections, several DFT with different exchange-correlation functional…

Surface (mathematics)DipoleMaterials scienceAb initio quantum chemistry methodsRelaxation (NMR)Density functional theoryPolarization (electrochemistry)Molecular physicsPerovskite (structure)IonMRS Proceedings
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Metal clusters on an inert surface: A simple model

1997

The shapes of metal clusters (with 2 to 14 valence electrons) on an inert surface are studied with a simple model based on the ultimate jellium model. It is shown that within certain approximations the surface-cluster interaction can be described with an external potential in the Kohn-Sham method. No restrictions for the cluster geometry are imposed. The results show that depending on the strength of the interaction and on the size of the cluster, the ground state is either planar or three-dimensional, but in many cases both geometries are stable and there is a marked energy barrier between them. The results agree qualitatively with ab initio calculations of Na clusters on a NaCl(100) surfa…

Surface (mathematics)Magic number (programming)PlanarMaterials scienceAb initio quantum chemistry methodsJelliumPhysics::Atomic and Molecular ClustersCluster (physics)Atomic physicsValence electronGround stateMolecular physicsAtomic and Molecular Physics and Optics
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Ab InitioCalculations of the Atomic and Electronic Structure of SrZrO3(111) Surfaces

2012

The paper presents and discusses the results of calculations of surface relaxations and energetics for the polar (111) surface of SrZrO3 using a hybrid B3LYP description of exchange and correlation. On the (111) surface, I consider both Zr- and SrO3-terminations. For both Zr and SrO3-terminated SrZrO3 (111) surfaces upper layer atoms relax inwards. The second layer atoms, with the sole exception of Zr-terminated SrZrO3 (111) surface Sr atom, relax outwards. The calculated surface relaxation energy for Zr-terminated SrZrO3 (111) surface is almost sixteen times larger, than the surface relaxation energy for SrO3-terminated SrZrO3 (111) surface. The surface energy for Zr-terminated SrZrO3 (111…

Surface (mathematics)Materials scienceAb initio quantum chemistry methodsAtomPolarRelaxation (physics)Surface phononElectronic structureAtomic physicsCondensed Matter PhysicsMolecular physicsSurface energyElectronic Optical and Magnetic MaterialsFerroelectrics
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First-Principles Calculations of SrZrO3 (001) Surfaces

2011

The results of calculations of surface relaxations, rumplings, and charge distribution for the SrZrO3 (001) surface using ab initio code CRYSTAL and a hybrid description of exchange and correlation are presented. Both SrO and ZrO2 terminations of the SrZrO3 (001) surface are considered. On the (001) surfaces all upper and third layer atoms relax inward, while outward relaxations of all atoms in the second layer are found with the sole exception of SrO-terminated SrZrO3 (001) surface second layer O atom. Calculated surface rumpling for the SrO-terminated SrZrO3 (001) surface 6.77% of the lattice constant is by a factor of ten larger than the surface rumpling for the ZrO2-terminated SrZrO3 (0…

Surface (mathematics)Materials scienceAb initioCharge densityCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCrystalLattice constantChemical bondControl and Systems EngineeringAb initio quantum chemistry methodsAtomMaterials ChemistryCeramics and CompositesElectrical and Electronic EngineeringAtomic physicsIntegrated Ferroelectrics
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Ab initiocalculations of theSrTiO3(110) polar surface

2004

Results of ab initio Hartree-Fock calculations for the SrTiO3 ~110! polar surface are discussed. We have calculated the surface energies, near-surface atomic displacements for four possible terminations ~TiO, Sr, and two kinds of O terminations! as well as Mulliken atomic charges and dipole moments of atoms characterizing their polarization, and the atomic bond populations. We predict a considerable increase of the TiuO chemical bond covalency near the ~110! surface, as compared to both the bulk and the ~100! surface. The O-terminated ~110! surface has surface energy close to that for ~100!, which indicates that both ~110! and ~100! SrTiO3 surfaces can coexist in polycrystals and perovskite…

Surface (mathematics)Materials scienceAb initioCondensed Matter PhysicsPolarization (waves)Surface energyElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceDipoleChemical bondAb initio quantum chemistry methodsPhysics::Atomic PhysicsAtomic physicsPerovskite (structure)Physical Review B
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