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Intercalated architecture of MA(2)Z(4) family layered van der Waals materials with emerging topological, magnetic and superconducting properties

The search for new two-dimensional monolayers with diverse electronic properties has attracted growing interest in recent years. Here, we present an approach to construct MA(2)Z(4) monolayers with a septuple-atomic-layer structure, that is, intercalating a MoS(2)-type monolayer MZ(2) into an InSe-ty...

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Detalles Bibliográficos
Autores principales: Wang, Lei, Shi, Yongpeng, Liu, Mingfeng, Zhang, Ao, Hong, Yi-Lun, Li, Ronghan, Gao, Qiang, Chen, Mingxing, Ren, Wencai, Cheng, Hui-Ming, Li, Yiyi, Chen, Xing-Qiu
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8060390/
https://www.ncbi.nlm.nih.gov/pubmed/33883547
http://dx.doi.org/10.1038/s41467-021-22324-8
Descripción
Sumario:The search for new two-dimensional monolayers with diverse electronic properties has attracted growing interest in recent years. Here, we present an approach to construct MA(2)Z(4) monolayers with a septuple-atomic-layer structure, that is, intercalating a MoS(2)-type monolayer MZ(2) into an InSe-type monolayer A(2)Z(2). We illustrate this unique strategy by means of first-principles calculations, which not only reproduce the structures of MoSi(2)N(4) and MnBi(2)Te(4) that were already experimentally synthesized, but also predict 72 compounds that are thermodynamically and dynamically stable. Such an intercalated architecture significantly reconstructs the band structures of the constituents MZ(2) and A(2)Z(2), leading to diverse electronic properties for MA(2)Z(4), which can be classified according to the total number of valence electrons. The systems with 32 and 34 valence electrons are mostly semiconductors. Whereas, those with 33 valence electrons can be nonmagnetic metals or ferromagnetic semiconductors. In particular, we find that, among the predicted compounds, (Ca,Sr)Ga(2)Te(4) are topologically nontrivial by both the standard density functional theory and hybrid functional calculations. While VSi(2)P(4) is a ferromagnetic semiconductor and TaSi(2)N(4) is a type-I Ising superconductor. Moreover, WSi(2)P(4) is a direct gap semiconductor with peculiar spin-valley properties, which are robust against interlayer interactions. Our study thus provides an effective way of designing septuple-atomic-layer MA(2)Z(4) with unusual electronic properties to draw immediate experimental interest.