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共价有机框架中的类利布晶格及其斯托纳铁磁性。

A Lieb-like lattice in a covalent-organic framework and its Stoner ferromagnetism.

作者信息

Jiang Wei, Huang Huaqing, Liu Feng

机构信息

Department of Materials Science and Engineering, University of Utah, Salt Lake City, UT, 84112, USA.

Department of Electrical and Computer Engineering, University of Minnesota, Minneapolis, MN, 55455, USA.

出版信息

Nat Commun. 2019 May 17;10(1):2207. doi: 10.1038/s41467-019-10094-3.

Abstract

Lieb lattice has been extensively studied to realize ferromagnetism due to its exotic flat band. However, its material realization has remained elusive; so far only artificial Lieb lattices have been made experimentally. Here, based on first-principles and tight-binding calculations, we discover that a recently synthesized two-dimensional sp carbon-conjugated covalent-organic framework (spc-COF) represents a material realization of a Lieb-like lattice. The observed ferromagnetism upon doping arises from a Dirac (valence) band in a non-ideal Lieb lattice with strong electronic inhomogeneity (EI) rather than the topological flat band in an ideal Lieb lattice. The EI, as characterized with a large on-site energy difference and a strong dimerization interaction between the corner and edge-center ligands, quenches the kinetic energy of the usual dispersive Dirac band, subjecting to an instability against spin polarization. We predict an even higher spin density for monolayer spc-COF to accommodate a higher doping concentration with reduced interlayer interaction.

摘要

由于其奇特的平带,利布晶格已被广泛研究以实现铁磁性。然而,其材料实现仍然难以捉摸;到目前为止,仅通过实验制备了人工利布晶格。在此,基于第一性原理和紧束缚计算,我们发现最近合成的二维sp碳共轭共价有机框架(spc-COF)代表了一种类利布晶格的材料实现。掺杂时观察到的铁磁性源于具有强电子不均匀性(EI)的非理想利布晶格中的狄拉克(价)带,而非理想利布晶格中的拓扑平带。EI表现为较大的在位能差以及角部和边缘中心配体之间强烈的二聚化相互作用,它淬灭了通常色散狄拉克带的动能,从而导致对自旋极化的不稳定性。我们预测单层spc-COF具有更高的自旋密度,以适应更高的掺杂浓度并减少层间相互作用。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ef5e/6525167/0985428427ae/41467_2019_10094_Fig1_HTML.jpg

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