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Vacancy-induced magnetic states in TiO2 surfaces

  1. 1.
    0573489 - ÚFM 2024 RIV US eng J - Journal Article
    Friák, Martin - Nhu, T. Q. - Meduňa, M. - Gazdová, K. - Pavlů, J. - Munzar, D. - Hong, N. H.
    Vacancy-induced magnetic states in TiO2 surfaces.
    Journal of Applied Physics. Roč. 134, č. 1 (2023), č. článku 013902. ISSN 0021-8979. E-ISSN 1089-7550
    Research Infrastructure: CzechNanoLab - 90110
    Institutional support: RVO:68081723
    Keywords : TiO2 * magnetism * defects
    OECD category: Condensed matter physics (including formerly solid state physics, supercond.)
    Impact factor: 3.2, year: 2022
    Method of publishing: Open access
    https://pubs.aip.org/aip/jap/article-abstract/134/1/013902/2901571/Vacancy-induced-magnetic-states-in-TiO2-surfaces?redirectedFrom=fulltext

    We present a combined experimental and theoretical study of surface-related magnetic states in TiO2. Our experiments on nano-sized thin
    films of pure TiO2 have suggested that the observed room-temperature magnetism originates from defects, in particular, from the surface
    of thin films as well as from point defects, such as oxygen vacancies located mainly at the surface. Clarifying this phenomenon is very
    important for harnessing magnetic properties of pristine TiO2 films in future spintronic applications but a detailed experimental investiga tion is very demanding. Therefore, quantum-mechanical density functional theory calculations were performed for (i) bulk anatase TiO2,
    (ii) bulk-like TiO2-terminated vacancy-free (001) surfaces, (iii) vacancy-containing TiO-terminated (001) surfaces, (iv) TiO0:75-terminated
    (001) surfaces with additional 25% surface oxygen vacancies, as well as (v) oxygen-terminated (001)-surfaces. Our fixed-spin-moment calcu lations identified both the bulk and the bulk-like terminated vacancy-free TiO2-terminated (001) surfaces as non-magnetic. In contrast,
    oxygen vacancies in the case of TiO-terminated and TiO0:75-terminated (001) surfaces lead to ferromagnetic and rather complex ferrimag netic states, respectively. The spin-polarized atoms are the Ti atoms (due to the d-states) located in the surface and sub-surface atomic
    planes. Last, the O-terminated surfaces are also magnetic due to the surface and sub-surface oxygen atoms and sub-surface Ti atoms
    (but their surface energy is high).
    Permanent Link: https://hdl.handle.net/11104/0343927

     
     
Number of the records: 1  

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