Hydrogen on the Fe (1̄12) surface and hydrogen pairs near bcc mixed (a/2)[11̄1] dislocation: Electronic structure

The bonding of H and H-H pairs to Fe is analyzed using qualitative electronic calculations in the framework of the atom superposition and electron delocalization molecular orbital cluster (ASED-MO) method. The changes in the electronic structure of bcc Fe upon introduction of a (a/2)[11̄1] mixed dis...

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Detalles Bibliográficos
Autores principales: Juan, A., Brizuela, G., Irigoyen, B., Gesari, S.
Formato: JOUR
Materias:
Acceso en línea:http://hdl.handle.net/20.500.12110/paper_00396028_v466_n1-3_p97_Juan
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Sumario:The bonding of H and H-H pairs to Fe is analyzed using qualitative electronic calculations in the framework of the atom superposition and electron delocalization molecular orbital cluster (ASED-MO) method. The changes in the electronic structure of bcc Fe upon introduction of a (a/2)[11̄1] mixed dislocation are compared with Fe surfaces. A comparison is drawn with H adsorption at the Fe (1̄12) surface. H in the bulk Fe with dislocations prefers to be near the dislocation core, acting as a trap for H. The Fe atoms are initially more strongly bonded to each other as a consequence of a dislocation introduction (an internal surface); the Fe-H interaction decreases the Fe-Fe bond strength. The H effect is limited to its first Fe neighbor. An analysis of the orbital interaction reveals that the Fe-H bonding involves mainly the Fe 4s and H 1s orbitals. A second H is approximated to the minimum energy region when one H is previously positioned. The orbital population analysis reveals some H-H association. The H-Fe interaction is compared with that produced in other defects (vacancies and stacking faults).