Recently, a new two-dimensional (2D) layered MoSiN has been successfully synthesized by chemical vapor deposition without knowing the 3D counterparts [ 2020, 369, 670-674]. The unique septuple-atomic-layer structure and diverse composition of MoSiN have drawn tremendous interest in studying 2D MAZ systems based on the MoSiN structure. As an emerging family of 2D materials, MAZ materials exhibit a wide range of properties and excellent tunability, making them highly promising for various applications.
View Article and Find Full Text PDFTwo-dimensional metal borides have received attention as high performance battery anode materials. During the practical application, the 2D surface terminalization is an inevitable problem. This study employs first-principles calculations to investigate the termination of the MgB monolayer with O, H, F, and Cl groups.
View Article and Find Full Text PDFWhen two-dimensional (2D) materials are stacked into van der Waals structures, interlayer electronic coupling can induce excellent properties in energy storage materials. Here, we investigate the interlayer coupling of the FeN/FeB heterojunction as an anode material, which is constructed using vertically planar FeN and puckered FeB nanosheets. These structures were searched by the CALYPSO method and computed by density functional theory calculations.
View Article and Find Full Text PDFDesigning novel multifunctional materials at the nanoscale is vitally important for flexible electronics. Here, we have uncovered a two-dimensional metal dichalcogenide PbS with intriguing negative Poisson ratio behavior and favorable optical and photocatalytic water splitting properties. The calculations indicate that the Poisson ratio of the PbS monolayer is -0.
View Article and Find Full Text PDFJ Phys Chem Lett
September 2021
We perform a first-principles study and identify two intriguing ferromagnets, hollow-FeN (H-FeN) and bridge-FeN (B-FeN) monolayers, by extensive structural searches. Both H-FeN and B-FeN nanosheets are buckled triangular lattices with a similar motif, but they are distinguishable by the positions of N atoms. The magnetic and electronic properties show that H-FeN is a low-spin ferromagnet; in contrast, B-FeN is a high-spin ferromagnet, which originates from the 3d orbital splitting of the Fe atom due to the low/high symmetric crystal field.
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