A theoretical study of H absorption at a Fe(110)–Pd(100) interface and Fe–Pd alloys

P. JASEN; E. GONZÁLEZ; N. J. CASTELLANI; A. JUAN

JOURNAL OF MATERIALS SCIENCE

Springer Netherlands

Lugar: Amsterdam; Año: 2005 vol. 40 p. 2775 - 2782

0022-2461

The electronic structure and bonding at a Fe(110)–Pd(100) interface was theoretically analyzed in the framework of semi-empirical quantum chemical calculations. The Fe–Pd interface was  modeled by a Fe74Pd74 cluster and a Fe–Pd six layer slab. The extended H¨ uckel tight binding (EHTB) method and its modifications, including repulsive interactions, were used to calculate the interfacial adhesion and the H-absorption energy. The energetic minimum position for H is found at the Fe–Pd interface closer to the Pd layer. The interfacial Fe–Pd distance result to be 1.73 ° A where Fe–Pd develops a strong bonding interaction. An important metal–metal adhesion was also found. The changes in the Density of States (DOS) and the Crystal Orbital Overlap Population (COOP) were compared in different structures: clusters, slab and two types of Fe–Pd alloys. The H as an impurity is responsible for a Fe–Fe and Pd–Pd bond weakening. However, the H effect is much less detrimental for the Fe–Pd bonds at the interface. When H is located at interstitial sites in bulk Fe–Pd alloys, the Pd–Pd overlap population shows a notorious decrease in the case of fcc structures while for fct structures the change is only 12%. The intermetallic bonding was also weakened as compared with the pure alloys. The objective of this work is to bring a plausible explanation to the null permeability to hydrogen in Pd-coated Fe films.e74Pd74 cluster and a Fe–Pd six layer slab. The extended H¨ uckel tight binding (EHTB) method and its modifications, including repulsive interactions, were used to calculate the interfacial adhesion and the H-absorption energy. The energetic minimum position for H is found at the Fe–Pd interface closer to the Pd layer. The interfacial Fe–Pd distance result to be 1.73 ° A where Fe–Pd develops a strong bonding interaction. An important metal–metal adhesion was also found. The changes in the Density of States (DOS) and the Crystal Orbital Overlap Population (COOP) were compared in different structures: clusters, slab and two types of Fe–Pd alloys. The H as an impurity is responsible for a Fe–Fe and Pd–Pd bond weakening. However, the H effect is much less detrimental for the Fe–Pd bonds at the interface. When H is located at interstitial sites in bulk Fe–Pd alloys, the Pd–Pd overlap population shows a notorious decrease in the case of fcc structures while for fct structures the change is only 12%. The intermetallic bonding was also weakened as compared with the pure alloys. The objective of this work is to bring a plausible explanation to the null permeability to hydrogen in Pd-coated Fe films.