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      (CrAs)₃(MnAs)₃(110) 초격자의 전자구조와 자성에 대한 제일원리 연구

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      https://www.riss.kr/link?id=A76076283

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      다국어 초록 (Multilingual Abstract)

      We investigated the magnetism and electronic structures for the layered structures consisting of (110) layers of zinc-blende CrAs and MnAs. We calculated the electronic structures for (CrAs)₃(MnAs)₃(110) superlattice consisted of alternating three layers of CrAs(110) and MnAs(110) by the full-potential linearized augmented plane wave (FLAPW) method. The calculated magnetic moment of Cr in interface layer (3.07 μ<SUB>B</SUB>) was slightly larger than that of Cr atom in center layer (3.06 μ<SUB>B</SUB>), while that of interface Mn atom (3.74 μ<SUB>B</SUB>) was slightly smaller than the value of Mn atom in center layer (3.76 μ<SUB>B</SUB>). The electronic structure and half-metallicity in this superlattice were discussed using the calculated density of states.
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      We investigated the magnetism and electronic structures for the layered structures consisting of (110) layers of zinc-blende CrAs and MnAs. We calculated the electronic structures for (CrAs)₃(MnAs)₃(110) superlattice consisted of alternating three...

      We investigated the magnetism and electronic structures for the layered structures consisting of (110) layers of zinc-blende CrAs and MnAs. We calculated the electronic structures for (CrAs)₃(MnAs)₃(110) superlattice consisted of alternating three layers of CrAs(110) and MnAs(110) by the full-potential linearized augmented plane wave (FLAPW) method. The calculated magnetic moment of Cr in interface layer (3.07 μ<SUB>B</SUB>) was slightly larger than that of Cr atom in center layer (3.06 μ<SUB>B</SUB>), while that of interface Mn atom (3.74 μ<SUB>B</SUB>) was slightly smaller than the value of Mn atom in center layer (3.76 μ<SUB>B</SUB>). The electronic structure and half-metallicity in this superlattice were discussed using the calculated density of states.

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