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Ferromagnetic-antiferromagnetic coexisting ground state and exchange bias effects in MnBi(4)Te(7) and MnBi(6)Te(10)
Natural superlattice structures MnBi(2)Te(4)(Bi(2)Te(3))(n) (n = 1, 2, ...), in which magnetic MnBi(2)Te(4) layers are separated by nonmagnetic Bi(2)Te(3) layers, hold band topology, magnetism and reduced interlayer coupling, providing a promising platform for the realization of exotic topological q...
Autores principales: | , , , , , , , , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9741634/ https://www.ncbi.nlm.nih.gov/pubmed/36496444 http://dx.doi.org/10.1038/s41467-022-35184-7 |
Sumario: | Natural superlattice structures MnBi(2)Te(4)(Bi(2)Te(3))(n) (n = 1, 2, ...), in which magnetic MnBi(2)Te(4) layers are separated by nonmagnetic Bi(2)Te(3) layers, hold band topology, magnetism and reduced interlayer coupling, providing a promising platform for the realization of exotic topological quantum states. However, their magnetism in the two-dimensional limit, which is crucial for further exploration of quantum phenomena, remains elusive. Here, complex ferromagnetic-antiferromagnetic coexisting ground states that persist down to the 2-septuple layers limit are observed and comprehensively investigated in MnBi(4)Te(7) (n = 1) and MnBi(6)Te(10) (n = 2). The ubiquitous Mn-Bi site mixing modifies or even changes the sign of the subtle interlayer magnetic interactions, yielding a spatially inhomogeneous interlayer coupling. Further, a tunable exchange bias effect, arising from the coupling between the ferromagnetic and antiferromagnetic components in the ground state, is observed in MnBi(2)Te(4)(Bi(2)Te(3))(n) (n = 1, 2), which provides design principles and material platforms for future spintronic devices. Our work highlights a new approach toward the fine-tuning of magnetism and paves the way for further study of quantum phenomena in MnBi(2)Te(4)(Bi(2)Te(3))(n) (n = 1, 2) as well as their magnetic applications. |
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