The effect of annealing and cooling on the structural properties of thin cobalt films possessing either hcp(0001) or fcc(100) crystalline arrangement is studied on clean and carbon-reconstructed W(110), respectively. The films grown on a clean W(110) crystal present a surface with hexagonal symmetry and undergo the well-known hcp–fcc structural transition upon annealing to temperatures higher than 700 K, while after cooling down to room temperature, the film is characterized by a laterally heterogeneous morphology featuring different stacking configurations. On carbide-covered W(110), Co grows, instead, in an fcc(100) arrangement with a high level of disorder, for which annealing leads to an improved crystalline order. Further annealing to above 900 K induces an irreversible transition from fcc(100) to hcp(0001) stacking via domain nucleation and growth on a micrometer scale. This recrystallization process is accompanied by a change in the film’s chemical composition and magnetic structure. The excess carbon resulting from recrystallization leads to the growth of micrometer-sized graphene islands on top of the hcp regions.
Thermally Induced Chemical and Structural Transformations in Thin Cobalt Films
Brondin, Carlo Alberto;
2024-01-01
Abstract
The effect of annealing and cooling on the structural properties of thin cobalt films possessing either hcp(0001) or fcc(100) crystalline arrangement is studied on clean and carbon-reconstructed W(110), respectively. The films grown on a clean W(110) crystal present a surface with hexagonal symmetry and undergo the well-known hcp–fcc structural transition upon annealing to temperatures higher than 700 K, while after cooling down to room temperature, the film is characterized by a laterally heterogeneous morphology featuring different stacking configurations. On carbide-covered W(110), Co grows, instead, in an fcc(100) arrangement with a high level of disorder, for which annealing leads to an improved crystalline order. Further annealing to above 900 K induces an irreversible transition from fcc(100) to hcp(0001) stacking via domain nucleation and growth on a micrometer scale. This recrystallization process is accompanied by a change in the film’s chemical composition and magnetic structure. The excess carbon resulting from recrystallization leads to the growth of micrometer-sized graphene islands on top of the hcp regions.I documenti in ARCA sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.