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Vacancy filled nickel‐cobalt‐titanate thin films
Author(s) -
Fujioka Yukari,
Frantti Johannes,
Rouleau Christopher,
Puretzky Alexander,
Meyer Harry M.
Publication year - 2017
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.201600799
Subject(s) - octahedron , materials science , crystallography , corundum , cobalt , vacancy defect , raman spectroscopy , crystal structure , chemistry , metallurgy , optics , physics
Single phase nickel‐cobalt‐titanate thin films with a formula A 1+2 x Ti 1− x O 3 , where A is Ni 2+ ,Co 2+ , and −0.25 < x < 1, were grown by pulsed laser deposition on sapphire substrates. There is a large window in which Ni/Co ratio and x can be chosen independently, allowing a control of properties by the synthesis. In the prototype ilmenite and corundum structures one third of the octahedra are vacant. The reported structure is obtained by filling vacant octahedra ( x > 0) or emptying filled octahedra ( x < 0). Films with x = 1 have all octahedra filled. X‐ray photoelectron spectroscopy, X‐ray diffraction measurements and Raman scattering techniques were applied to address the structure as a function of x . Data collected on samples with x ≈ 1 are interpreted in terms of hexagonal P 6 3 / mmc space group. The hexagonal structure was obtained when films contained both Ni and Co: pure cobalt oxide thin films possessed the spinel structure. Two factors controlling the magnetism and crystal distortion are identified: a direct overlap between the adjacent cation d ‐orbitals resulting in a bond formation and magnetic interactions, and x controlling the cation shift toward the vacant octahedron. The displacement decreases and the symmetry increases with increasing x . When x ≈ 1 the cations prefer octahedron center positions.
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