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Room temperature ferromagnetism in metallic Ti(1−x)V(x)O(2) thin films
Transition metal doped TiO(2) diluted magnetic semiconductors have attracted considerable interest due to their room temperature ferromagnetism. However, most TiO(2) films are highly insulating, and thus the magnetic properties can not be controlled by tuning the carrier concentration. This will lim...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2018
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9085575/ https://www.ncbi.nlm.nih.gov/pubmed/35548233 http://dx.doi.org/10.1039/c8ra06343e |
Sumario: | Transition metal doped TiO(2) diluted magnetic semiconductors have attracted considerable interest due to their room temperature ferromagnetism. However, most TiO(2) films are highly insulating, and thus the magnetic properties can not be controlled by tuning the carrier concentration. This will limit their application in controlling magnetization via electrical gating. Here, we deposit rutile Ti(1−x)V(x)O(2) (x = 0.03 and 0.05) films with the thickness between 30 and 245 nm by the pulsed laser deposition technique, and observe an obvious room temperature ferromagnetic behavior in all films. The high resolution X-ray photoelectron spectroscopy results indicate that V substituting Ti(4+) ions in the TiO(2) lattice, with the +3 valence state having two unpaired d electrons, is responsible for the local spin. More importantly, the systemic investigations of transport properties for Ti(1−x)V(x)O(2) films reveal that the films are n-type and have metallic conductivity with a carrier density of about 10(20)/cm(3). Further studies suggest that the oxygen vacancies play a dual role of contributing to the metallic conductivity of the Ti(1−x)V(x)O(2) films, and also providing the free electrons to mediate the long-range ferromagnetic coupling between two magnetic polarons. These findings may offer promise for gate-tunable ferromagnetism in future semiconductor spintronics. |
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