Search results for "Length"

showing 10 items of 2188 documents

Electronic Properties of Mixed-Valence Manganates:  The Role of Mn Substitutional Defects

2002

Single-phase perovskites in the solid solution series La0.7+yA0.3-yMn1-xMxO3 (with 0.00 ≤ x ≤ 0.10; A = Sr2+, M = Cu2+, Zn2+, Sc3+, Cr3+, Co3+, and Ga3+; A = Ba2+, M = Cu2+, Zn2+, and Sc3+) have been prepared via the acetic acid solutions freeze-drying method. This soft procedure makes possible strict stoichiometric control, and the synthetic variables allow one to maintain a constant proportion of Mn4+ (ca. 32%) in the 47 compounds prepared. In this way, the concentration of cationic vacancies at A and B sites is practically negligible in all cases. X-ray powder diffraction patterns corresponding to the 47 compounds have been completely indexed with rhombohedral perovskite cells. The cryst…

Bond lengthCrystallographyMaterials scienceValence (chemistry)General Chemical EngineeringMaterials ChemistryCationic polymerizationGeneral ChemistryCrystal structurePowder diffractionStoichiometryElectronic propertiesPerovskite (structure)Chemistry of Materials
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Bis(dimethylammonium) pentachloroantimonate(III), on the deformation of the octahedral coordination of Sb III

1998

The structure of the title compound, [NH2(CH3)2]2SbCl5, was determined at 295 and 85 K. It consists of polymeric (SbCl52−)n chains composed of deformed SbCl63− octahedra connected by corners and dimethylammonium cations. The temperature dependence of the Sb–Cl bond lengths is discussed. It is argued that the deformation of the octahedral coordination of the SbIII atom is caused by electrostatic interaction/hydrogen bonds.

Bond lengthCrystallographyOctahedronHydrogen bondChemistryInorganic chemistryAtomMoleculeGeneral MedicineCrystal structureDeformation (meteorology)General Biochemistry Genetics and Molecular BiologyElectrostatic interactionActa Crystallographica Section C-Crystal Structure Communications
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Variable-temperature X-ray crystal structure determinations of {Fe[tren(6-Mepy)3]}(ClO4)2and {Zn[tren(6-Mepy)3]}(ClO4)2compounds: correlation of the …

2007

Variable-temperature X-ray crystal structure determinations (80–330 K) on compounds {Fe[tren(6-Mepy)3]}(ClO4)2(1-Fe) {tren(6-Mepy)3is tris[3-aza-4-(6-methyl-2-pyridyl)but-3-enyl]amine} and {Zn[tren(6-Mepy)3]}(ClO4)2(1-Zn) {tren(6-Mepy)3is tris[3-aza-4-(6-methyl-2-pyridyl)but-3-enyl]amine} were carried out together with a detailed analysis of the unit-cell volume and parameters in the spin transition region for (1-Fe). Both compounds crystallize in the monoclinic system and retained the space groupP21/cat all measured temperatures. The Fe and Zn atoms are surrounded by six N atoms belonging to imine groups and pyridine groups of the trifurcated ligand, adopting a pseudo-octahedral symmetry. …

Bond lengthCrystallographySpin crossoverChemistryMössbauer spectroscopySpin transitionCrystal structureMole fractionMagnetic susceptibilityGeneral Biochemistry Genetics and Molecular BiologyMonoclinic crystal systemJournal of Applied Crystallography
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Relativistic coupled cluster calculations of the electronic structure of KrH+, XeH+ and RnH+

2012

Potential energy curves of NgH+ cations (Ng = Kr, Xe, Rn) were obtained by using four-component relativistic CCSD(T) coupled cluster calculations. Dissociation energies, equilibrium bond lengths, electronic properties, such as dipole moments and electric field gradients at the nuclei, and the related spectroscopic parameters of the electronic ground state have been determined. The results obtained for KrH+ and XeH+ are in good agreement with available experimental data, while those for RnH+ have been determined for the first time at this level of theory.

Bond lengthDipoleCoupled clusterChemistryElectric fieldRelativistic effects Coupled cluster Protonated noble gasesElectronic structurePhysical and Theoretical ChemistryAtomic physicsGround statePotential energyDissociation (chemistry)Theoretical Chemistry Accounts
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On the geometry of the HO3 radical

2008

Abstract We discuss the equilibrium structure of the hydrogen trioxy radical (HO3). The CCSD(T) geometry at the approximate basis set limit, in conjunction with the geometry obtained using the CCSDT method and a moderate basis set, suggests an equilibrium HO–OO bond length of approximately 1.59 A.

Bond lengthHydrogenchemistryStructure (category theory)General Physics and Astronomychemistry.chemical_elementMoleculeGeometryLimit (mathematics)Physical and Theoretical ChemistryBasis setChemical Physics
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High-pressure x-ray absorption study of GaTe including polarization

2000

The evolution of the local structure in GaTe under pressure is studied by x-ray absorption spectroscopy experiments at the Ga K-edge (10.368 keV) on oriented single crystals. Taking advantage of the linearly polarized character of synchrotron radiation, the pressure evolution of both the Ga-Te and the in-plane Ga-Ga bond lengths could be determined, in spite of the small amplitude of the latter. Our measurements show that both distances are much less compressible than what could be inferred from the bulk compressibility, which evidences a strong variation of Ga-Ga-Te and Te-Ga-Te angles under pressure. The Te-Te intralayer distance perpendicular to the layers is observed to increase with in…

Bond lengthMaterials scienceAbsorption spectroscopyExtended X-ray absorption fine structureLinear polarizationCompressibilitySynchrotron radiationAtomic physicsAnisotropyMolecular physicsX-ray absorption fine structure
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GERMANIUM DICARBIDE: EVIDENCE FOR A T−SHAPED GROUND STATE STRUCTURE

2017

The equilibrium structure of germanium dicarbide GeC2 has been an open question since the late 1950s. Although most high-level quantum calculations predict an L-shaped geometry, a T-shaped or even a linear geometry cannot be ruled out because of the very flat potential energy surface. By recording the rotational spectrum of this dicarbide using sensitive microwave and millimeter techniques, we unambiguously establish that GeC2 adopts a vibrationally averaged T-shaped structure in its ground state. From analysis of 14 isotopologues, a precise r0 structure has been derived, yielding a Ge–C bond length of 1.952(1) A and an apex angle of 38.7(2)°.

Bond lengthMaterials sciencechemistryPotential energy surfacechemistry.chemical_elementMillimeterIsotopologueGermaniumLinear molecular geometryGround stateMolecular physicsMicrowaveNuclear chemistryProceedings of the 72nd International Symposium on Molecular Spectroscopy
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An ab initio study of the tautomeric equilibria of the N-oxides of hydroxypyridines in the vapour phase

1993

Abstract An ab initio self-consistent field molecular orbital study of the N-oxides of hydroxypyridines has been carried out. The optimized structures have been obtained at the 6-31G ∗ level, and the energy values have been computed at the 6-31G ∗ and MP2-6-31G ∗ //6-31G ∗ levels. The tautomerization energies for the three couples of systems in the vapour phase have been evaluated.

Bond lengthMolecular geometryElectronic correlationChemistryAb initio quantum chemistry methodsComputational chemistryPhase (matter)Ab initioMolecular orbitalPhysical and Theoretical ChemistryCondensed Matter PhysicsBiochemistryTautomerJournal of Molecular Structure: THEOCHEM
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The deformation tensor ∊ of the spin transition in the mixed crystal [Fe0.46Zn0.54(ptz)6](BF4)2

2004

The conversion of the spin state of complexes exhibiting thermal spin crossover from the1A1low-spin (LS) state to the5T2high-spin (HS) state is accompanied by a deformation of the lattice due to the larger bond lengths in the HS state as compared with the LS state. In a previous work [Kuszet al.(2000).J. Appl. Cryst.33, 201–205], it has been shown that the deformation of the lattice, corrected for its temperature dependence, can be described by an almost temperature-independent tensor ∊ multiplied by the fraction of molecules in the HS state, γHS. Here the dependence of ∊ in a mixed single crystal of [Fe0.46Zn0.54(ptz)6](BF4)2(ptz = propyltetrazole) with a transition temperature near 110 K …

Bond lengthNuclear magnetic resonanceLattice constantSpin statesChemistrySpin crossoverExcited stateSpin transitionThermodynamicsCrystal structureGeneral Biochemistry Genetics and Molecular BiologyLIESSTJournal of Applied Crystallography
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Synthesis, crystal structure and magnetic properties of the complex [ReCl3(tppz)]·MeCN

2015

The reaction of the starting materials [ReIIICl3(MeCN)(PPh3)2] or [ReVOCl3(PPh3)2] with 2,3,5,6-tetrakis(2-pyridyl)pyrazine (tppz) in acetonitrile yielded the Re(III) complex [ReCl3(tppz)]·MeCN (1). This complex crystallizes in the monoclinic space group P21/n and its crystal structure consists of neutral mononuclear entities with meridional geometry of the chloride ligands, and the six-coordination of the Re(III) ion being completed by the tridentate tppz ligand. Each metal centre exhibits a highly distorted octahedral coordination with Re–Cl and Re–Ntppz bond lengths covering the ranges 2.3590(9)–2.3606(8) and 1.971(2)–2.096(2) A, respectively. The magnetic properties of 1 have been inves…

Bond lengthParamagnetismCrystallographyTetragonal crystal systemchemistry.chemical_compoundPyrazineChemistryGeneral Chemical EngineeringGeneral ChemistryCrystal structureGround stateMagnetic susceptibilityMonoclinic crystal systemRSC Advances
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