Search results for "Atom model"

showing 6 items of 6 documents

Modelling the carbon Snoek peak in ferrite: Coupling molecular dynamics and kinetic Monte-Carlo simulations

2008

Abstract Molecular statics, molecular dynamics and kinetic Monte-Carlo are used to model the carbon Snoek peak in ferrite. Using an interatomic EAM potential for the Fe–C system, saddle point energies for the diffusion of carbon have been evaluated under uniaxial stress by molecular statics. These energies have been reintroduced in a kinetic Monte-Carlo scheme to predict the repartition of carbon atoms in different octahedral sites. This repartition leads to an anelastic deformation calculated by molecular dynamics, which causes internal friction (the Snoek peak) for cyclic stress. This approach leads to quantitative predictions of the internal friction, which are in good agreement with exp…

General Computer ScienceMonte Carlo method[ SPI.MAT ] Engineering Sciences [physics]/MaterialsGeneral Physics and AstronomyThermodynamicsInteratomic potential02 engineering and technology[SPI.MAT] Engineering Sciences [physics]/MaterialsKinetic energy7. Clean energy01 natural sciences010305 fluids & plasmas[SPI.MAT]Engineering Sciences [physics]/MaterialsCondensed Matter::Materials ScienceMolecular dynamicsSaddle point0103 physical sciencesGeneral Materials ScienceKinetic Monte CarloComputingMilieux_MISCELLANEOUSEmbedded atom modelCondensed matter physicsChemistryGeneral Chemistry021001 nanoscience & nanotechnologyComputational MathematicsMechanics of MaterialsFerrite (magnet)0210 nano-technology
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Heteroepitaxial growth of Co on W(110) investigated by scanning tunneling microscopy

2003

We investigated the growth of Co submonolayers on bcc W(110) by scanning tunneling microscopy. Due to the strong Co-W bonding, monolayers of Co grow in equilibrium pseudomorphically on W(110) until the monolayer is almost completed. When excess atoms are deposited atop the pseudomorphic monolayer, it transforms to a close-packed (cp) monolayer with misfit dislocation lines parallel to $[11\ifmmode\bar\else\textasciimacron\fi{}0]$ (Nishiyama-Wassermann orientation). The structure of the cp monolayer, as concluded from atomically resolved STM images, deviates from the rigid hard-sphere model of a cp (111) layer. Details of the structure are compared to a structure model previously proposed by…

Materials sciencebusiness.industrylaw.inventionCrystallographyOpticslawMonolayerDislocationStructured modelScanning tunneling microscopebusinessLayer (electronics)Embedded atom modelBar (unit)Physical Review B
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(2S,3S)-2-(N,N-dibenzylamino)butane-1,3-diol refined using a multipolar atom model.

2008

The crystal structure of the title compound, C18H23NO2, was determined using the experimental library multipolar atom model. The refinement showed a significant improvement of crystallographic statistical indices when compared with a conventional spherical neutral atom refinement.

Models MolecularBenzylaminesEnergetic neutral atomMolecular Structure010405 organic chemistryChemistryStatistical indexDiolButaneGeneral MedicineCrystal structure010402 general chemistryCrystallography X-Ray01 natural sciencesGeneral Biochemistry Genetics and Molecular Biology3. Good health0104 chemical sciencesCrystallographychemistry.chemical_compound[CHIM.CRIS]Chemical Sciences/Cristallography[CHIM]Chemical SciencesButylene GlycolsComputingMilieux_MISCELLANEOUSAtom modelActa crystallographica. Section C, Crystal structure communications
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5-(3,4-Dimethoxybenzyl)-7-isopropyl-1,3,5-triazepane-2,6-dione acetonitrile solvate refined using a multipolar atom model

2010

International audience; The crystal structure of the title compound, C16H23N3O4·CH3CN, was refined using a multipolar atom model transferred from an experimental electron-density database. The refinement showed some improvement in crystallographic statistical indices compared with the independent atom model. The triazepane ring adopts a twist-boat conformation. In the crystal structure, the mol­ecule forms inter­molecular contacts with 14 different neighbours. There are two N-H...O and one C-H...O inter­molecular hydrogen bond.

Models MolecularStereochemistryMolecular ConformationCrystal structure010402 general chemistryRing (chemistry)Crystallography X-Ray01 natural sciencesGeneral Biochemistry Genetics and Molecular Biologychemistry.chemical_compoundBenzyl Compounds[CHIM.CRIS]Chemical Sciences/CristallographyMoleculeAcetonitrileQuantitative Biology::Biomolecules010405 organic chemistryChemistryHydrogen bondIntermolecular forceGeneral MedicineAzepines0104 chemical sciencesCrystallographySolubilityDimerizationIsopropylAtom model
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Trapping of hydrogen and helium at dislocations in tungsten: anab initiostudy

2017

Retention of plasma gas components such as hydrogen (H) isotopes and helium (He) is one of the limiting factors in selection of plasma facing materials for future thermonuclear fusion devices. Tungsten (W) is one of the promising candidates for such materials and was chosen for the divertor armor for International Thermonuclear Experimental Reactor (ITER) and the first wall material for the design of the demonstrational fusion power plant - DEMO. For the analytical estimation of accumulation of H/He components in tungsten, it is important to understand the relevant physical mechanisms of their trapping in the material and thoroughly parameterize them numerically. Experiments involving high …

Nuclear and High Energy PhysicsMaterials sciencetungstenH and He in Wtrapping at dislocationAb initiohelium02 engineering and technologyDFT7. Clean energy01 natural sciences010305 fluids & plasmasCondensed Matter::Materials ScienceAb initio quantum chemistry methodsVacancy defect0103 physical sciencesAtomPhysics::Atomic PhysicsplasmaEmbedded atom modelab initiomolecular staticsCharge density021001 nanoscience & nanotechnologyCondensed Matter Physics13. Climate actionhydrogenDislocationAtomic physics0210 nano-technologyBurgers vectordislocationsNuclear Fusion
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4-Benzoyl-3,4-dihydro-2 H -1,4-benzoxazine-2-carbonitrile: refinement using a multipolar atom model

2009

The structural model for the title compound, C(16)H(12)N(2)O(2), was refined using a multipolar atom model transferred from an experimental electron-density database. The refinement showed some improvements of crystallographic statistical indices when compared with a conventional spherical neutral-atom refinement. The title compound adopts a half-chair conformation. The amide N atom lies almost in the plane defined by the three neighbouring C atoms. In the crystal structure, molecules are linked by weak intermolecular C-H...O and C-H...pi hydrogen bonds.

Quantitative Biology::Biomolecules010405 organic chemistryChemistryHydrogen bondStatistical indexIntermolecular forceGeneral MedicineCrystal structure010402 general chemistry01 natural sciencesGeneral Biochemistry Genetics and Molecular Biology3. Good health0104 chemical scienceschemistry.chemical_compoundCrystallographyAmideAtom[CHIM.CRIS]Chemical Sciences/CristallographyMoleculePhysics::Atomic PhysicsComputingMilieux_MISCELLANEOUSAtom model
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