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First-principles study on the phase diagram and multiferroic properties of (SrCoO(3))(1)/(SrTiO(3))(1) superlattices
To design a multiferroic material at atomic scale, strong spin-lattice and charge-lattice couplings play crucial roles. Our first-principles calculation on (SrCoO(3))(1)/(SrTiO(3))(1) superlattices, with above coupling properties, yields a rich physical phase diagram as a function of epitaxial strai...
Autores principales: | , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2014
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3975234/ https://www.ncbi.nlm.nih.gov/pubmed/24699214 http://dx.doi.org/10.1038/srep04564 |
Sumario: | To design a multiferroic material at atomic scale, strong spin-lattice and charge-lattice couplings play crucial roles. Our first-principles calculation on (SrCoO(3))(1)/(SrTiO(3))(1) superlattices, with above coupling properties, yields a rich physical phase diagram as a function of epitaxial strain. In particular, a robust ferroelectric ferromagnetic insulator of Pc symmetry is stabilized at tensile strain Δa/a(0) = 0.86%–5.53%. The polarization can be as large as 36 μC/cm(2) and magnetic moment can reach 6μ(B) per unit cell. The magnetocrystalline anisotropy energy (0.16 meV/Co in (001) plane, 0.6 meV/Co in (100) plane) is comparable with that of TbMnO(3) compound and the magnetoelectric constant α (1.44 × 10(−3) Gaussian unit) is comparable with that of Co(3)B(7)O(13)Br compound. Our study suggests that epitaxially strained (SrCoO(3))(1)/(SrTiO(3))(1) superlattices not only offer an excellent candidate for multiferroic materials, but also demonstrate the half-metal and ferromagnetic insulator properties with potential application in spintronic devices. |
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