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The C–C pair in the vicinity of a bcc Fe bulk vacancy: electronic structure and bonding
Author(s) -
Simonetti S.,
Pronsato M. E.,
Brizuela G.,
Juan A.
Publication year - 2007
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/pssb.200642410
Subject(s) - vacancy defect , crystallography , octahedron , atomic orbital , chemistry , electronic structure , materials science , atomic physics , electron , computational chemistry , crystal structure , physics , quantum mechanics
C–Fe and C–C interactions near a bcc Fe vacancy were analysed using DFT calculations. A cell containing 14 atoms was used to simulate the local environment of the Fe vacancy. Carbon atoms were positioned in their local energy minimum configurations. The most stable positions for the C atoms in the vacancy region were found at about 1.23 Å from the vacancy centre and near the first nearest‐neighbour octahedral sites. Changes in the electronic structure of Fe atoms near a vacancy were analysed. Fe–Fe bonds surrounding the vacancy weaken their bond when the C atoms are present. This bond weakening is a consequence of C–Fe bond formation. The Fe–C interactions occur mainly via Fe 4s orbitals with a lesser participation of Fe 3p orbitals. There is an electron transfer to the C atoms from their Fe nearest neighbours. The C–C interaction was also analysed. For the C–C distance of 1.462 Å, there is a bonding between the C atoms. The C–C interaction is stronger than the C–Fe interactions. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)