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Effect of Growth Rate on the Crystal Orientation and Magnetization Performance of Cobalt Nanocrystal Arrays Electrodeposited from Aqueous Solution

The formation work of a two-dimensional hcp-Co (metallic cobalt crystal with hexagonal close packed structure) nucleus, W(hkl), was calculated by Pangarov’s theory. W(002) was estimated to be smaller than W(100) in a cathode potential range nobler than the transition potential, E(tra) (ca. −0.77 V v...

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Detalles Bibliográficos
Autores principales: Saeki, Ryusei, Ohgai, Takeshi
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6116207/
https://www.ncbi.nlm.nih.gov/pubmed/30042366
http://dx.doi.org/10.3390/nano8080566
Descripción
Sumario:The formation work of a two-dimensional hcp-Co (metallic cobalt crystal with hexagonal close packed structure) nucleus, W(hkl), was calculated by Pangarov’s theory. W(002) was estimated to be smaller than W(100) in a cathode potential range nobler than the transition potential, E(tra) (ca. −0.77 V vs. Ag/AgCl). To confirm the above estimation, ferromagnetic nanocomposite thick films, which contained (002) textured hcp-Co nanocrystal arrays, were synthesized by potentiostatic electrochemical reduction of Co(2+) ions in anodized aluminum oxide (AAO) nanochannel films with ca. 45 µm thickness. The aspect ratio of hcp-Co nanocrystals with a diameter of ca. 25 nm reached up to ca. 1800. Our experimental results revealed that the texture coefficient, TC(002), increased when decreasing the overpotential for hcp-Co electrodeposition by shifting the cathode potential nobler than E(tra). In a similar way, TC(002) increased sharply by decreasing the growth rate of the hcp-Co nanocrystals so that it was smaller than the transition growth rate, R(tra) (ca. 600 nm s(−1)). The perpendicular magnetization performance was observed in AAO nanocomposite films containing hcp-Co nanocrystal arrays. With increasing TC(002), the coercivity of the nanocomposite film increased and reached up to 1.66 kOe, with a squareness of ca. 0.9 at room temperature.