Search results for "bond"

showing 10 items of 3527 documents

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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Continuum Monte Carlo simulation of phase transitions in rod-like molecules at surfaces

1994

Stiff rod-like chain molecules with harmonic bond length potentials and trigonometric bond angle potentials are used to model Langmuir monolayers at high densities. One end of the rod-like molecules is strongly bound to a flat two-dimensional substrate which represents the air-water interface. A ground-state analysis is performed which suggests phase transitions between phases with and without collective uniform tilt. Large-scale off-lattice Monte Carlo simulations over a wide temperature range show in addition to the tilting transition the presence of a strongly constrained melting transition at high temperatures. The latter transition appears to be related to two-dimensional melting of th…

Bond lengthPhase transitionMolecular geometryMaterials scienceCondensed matter physicsLattice (order)Monte Carlo methodMonolayerGeneral Physics and AstronomyMoleculeAtmospheric temperature rangeIl Nuovo Cimento D
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A theoretical determination of the dissociation energy of the nitric oxide dimer

1994

Multi-reference CI methods have been applied to determine the dissociation energy and structure of thecis-N2O2 molecule. The convergence of the theoretical result has been checked with respect to a systematic expansion of the one-electron basis set and the multi-reference CI wave function. The best calculated value, 13.8 kJ/mol, is in agreement with the experimental value, 12.2 kJ/mol. It has been obtained with an extended ANO-type basis set [6s5p3d2f], including the effect of the basis set superposition error (BSSE) in the geometry optimization, and additional effects, such as the electron correlation of core electrons and relativistic corrections, using the average coupled pair functional…

Bond lengthPhysicsMolecular geometryElectronic correlationCore electronAb initio quantum chemistry methodsThermodynamicsChiropracticsPhysical and Theoretical ChemistryConfiguration interactionBond-dissociation energyBasis setTheoretica Chimica Acta
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AM1 prediction of the equilibrium geometry of Si60

1993

Abstract AM1 calculations have been carried out to determine the equilibrium geometry of Si 60 . The predicted I h geometry shows that bonds may be clearly identified as single (2.297 A) or aromatic (2.092 A). Several analogies and differences between Si 60 and C 60 are pointed out. Especially remarkable is the bigger size of the Si 60 cluster, which is predicted to have a radius 2 A larger than that of the C 60 cluster. Results are compared to other levels of theory.

Bond lengthSiliconChemistryComputational chemistryCluster (physics)General Physics and AstronomyMoleculeThermodynamicschemistry.chemical_elementElectronic structureRadiusPhysical and Theoretical ChemistryEquilibrium geometryChemical Physics Letters
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Experimental and theoretical studies of the molecular and crystal structures of trialkoxy- and chlorodialkoxy-stibanes

2001

The molecular structures of triisopropoxystibane, Sb((OPr)-Pr-i)(3), and chlorodiisopropoxystibane, SbCl((OPr)-Pr-i)(2), were determined in the solid state by single crystal X-ray diffraction. Sb((OPr)-Pr-i)(3) forms discrete centrosymmetric dimers in the solid state via Sb . . .O-Sb interactions, leading to pseudo trigonal bipyramidal configurations of the four co-ordinate Sb atoms, while SbCl((OPr)-Pr-i)(2) forms chains via Sb . . .O-Sb and Sb . . . Cl-Sb bridges, resulting in five-co-ordinate Sb atoms with pseudo octahedral configurations. Comparison of the solid state structures and the density functional optimized molecular structures of Sb(OMe)(3), SbCl(OMe)(2) and their dimers reveal…

Bond lengthTrigonal bipyramidal molecular geometryCrystallographychemistry.chemical_compoundOctahedronChemistryStereochemistryDimerGeneral ChemistryCrystal structureSingle crystalDissociation (chemistry)Natural bond orbital
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Octahedral distortion caused by hydrogen bonding in tris(diethylammonium) hexachloridoantimonate(III).

2010

The factors influencing the distortion of inorganic anions in the structures of chloridoantimonates(III) with organic cations, in spite of numerous structural studies on those compounds, have not been clearly described and separated. The title compound, [(C(2)H(5))(2)NH(2)](3)[SbCl(6)], consisting of isolated distorted [SbCl(6)](3-) octahedra that have C(3) symmetry and [(C(2)H(5))(2)NH(2)](+) cations, unequivocally shows the role played by hydrogen bonding in the geometry variations of inorganic anions. The organic cations, which are linked to the inorganic substructure through N-H...Cl hydrogen bonds, are clearly responsible for the distortion of the octahedral coordination of Sb(III) in …

Bond lengthTrischemistry.chemical_compoundCrystallographychemistryOctahedronHydrogen bondDistortionInorganic chemistrySubstructureGeneral MedicineCrystal structureGeneral Biochemistry Genetics and Molecular BiologyActa crystallographica. Section C, Crystal structure communications
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Analysis of the CIPSI/DCCI approach to characterize the HF AND F2 single bond

1990

Abstract The aim of the present work is to account for the main differential correlation contributions occurring during the bond breaking process of HF and F2 molecules in an accurate and inexpensive way. Starting from the dissociation-consistent configuration interaction (DCCI) scheme by Goddard and co-workers the corresponding contributions are evaluated within the framework reported by Malrieu and co-workers, namely configuration interaction by perturbation with multiconfigurational zeroth-order wavefunction selected by iterative process (CIPSI). In addition, the DCCI scheme has been improved by introducing the dispersion effects associated with the valence MOs adjacent to the bond. The …

Bond lengthValence (chemistry)Electronic correlationComputational chemistryChemistryGeneral Physics and AstronomySingle bondElectronic structurePhysical and Theoretical ChemistryConfiguration interactionWave functionMolecular physicsDiatomic moleculeChemical Physics
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