z-logo
Premium
Quantum‐Mechanical ab initio Investigation of the Transition‐Metal Compounds OsO 4 , OsO 3 F 2 , OsO 2 F 4 , OsOF 6 , and OsF 8
Author(s) -
Veldkamp Achim,
Frenking Gernot
Publication year - 1993
Publication title -
chemische berichte
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.667
H-Index - 136
eISSN - 1099-0682
pISSN - 0009-2940
DOI - 10.1002/cber.19931260609
Subject(s) - chemistry , ab initio , bond length , ab initio quantum chemistry methods , ionic bonding , molecular geometry , hypersurface , symmetry (geometry) , atomic physics , chemical bond , crystallography , molecule , crystal structure , physics , geometry , ion , mathematical analysis , mathematics , organic chemistry
The equilibrium geometries of OsO 4 , OsO 3 F 2 , OsO 2 F 4 and OsF 8 are theoretically predicted by using quantum‐mechanical ab initio methods at the Hartree‐Fock and MP2 level of theory employing quasi‐relativistic pseudopotentials for Os and 3‐21G and 6‐31G(d) basis sets for O and F. A comparison of the calculated geometries and vibrational frequencies with available experimental results shows a good agreement. The energy minimum structure for OsO 4 has T d symmetry, for OsO 3 F 2 it has D 3 h symmetry, for OsO 2 F 4 C 2v symmetry with cis 1‐coordinated oxygen atoms, and for OsF 8 a D 2d symmetry with two different Os – F bond lengths is predicted. OsOF 6 is not a minimum on the potential energy hypersurface. The calculation of the thermodynamic stabilities indicates that the Os – F bond in OsF 8 is clearly weaker than in OsO 3 F 2 , OsO 2 F 4 and in OsF 6 . It will be very difficult to observe OsF 8 experimentally. The analysis of the electronic structure shows that the Os – O bond is partly covalent, while the Os – F bonds are mainly ionic.

This content is not available in your region!

Continue researching here.

Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom