Jiang Wei, Zhang Shunhong, Wang Zhengfei, Liu Feng, Low Tony
Department of Electrical & Computer Engineering, University of Minnesota, Minneapolis, Minnesota 55455, United States.
International Center for Quantum Design of Functional Materials (ICQD), Hefei National Laboratory for Physical Sciences at Microscale, and CAS Center For Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, Anhui 230026, China.
Nano Lett. 2020 Mar 11;20(3):1959-1966. doi: 10.1021/acs.nanolett.9b05242. Epub 2020 Feb 25.
Topological properties of the Lieb lattice, i.e., the edge-centered square lattice, have been extensively studied and are, however, mostly based on theoretical models without identifying real material systems. Here, based on tight-binding and first-principles calculations, we demonstrate the Lieb-lattice features of the experimentally synthesized phthalocyanine-based metal-organic framework (MPc-MOF), which holds various intriguing topological phase transitions through band engineering. First, we show that the MPc-MOFs indeed have a peculiar Lieb band structure with 1/3 filling, which has been overlooked because of its unconventional band structure deviating from the ideal Lieb band. The intrinsic MPc-MOF presents a trivial insulating state, with its gap size determined by the on-site energy difference (Δ) between the corner and edge-center sites. Through either chemical substitution or physical strain engineering, one can tune Δ to close the gap and achieve a topological phase transition. Specifically, upon closing the gap, topological semimetallic/insulating states emerge from nonmagnetic MPc-MOFs, while magnetic semimetal/Chern insulator states arise from magnetic MPc-MOFs, respectively. Our discovery greatly enriches our understanding of the Lieb lattice and provides a guideline for experimental observation of the Lieb-lattice-based topological states.
李布晶格(即边心正方晶格)的拓扑性质已得到广泛研究,然而,这些研究大多基于理论模型,并未确定实际的材料体系。在此,基于紧束缚和第一性原理计算,我们展示了实验合成的酞菁基金属有机框架(MPc-MOF)的李布晶格特征,该框架通过能带工程展现出各种有趣的拓扑相变。首先,我们表明MPc-MOF确实具有填充率为1/3的独特李布能带结构,由于其非常规的能带结构偏离理想李布能带,该结构一直被忽视。本征MPc-MOF呈现出平凡绝缘态,其能隙大小由角位点和边心位点之间的在位能量差(Δ)决定。通过化学取代或物理应变工程,均可调节Δ以关闭能隙并实现拓扑相变。具体而言,在关闭能隙时,非磁性MPc-MOF会出现拓扑半金属/绝缘态,而磁性MPc-MOF则分别出现磁半金属/陈绝缘体态。我们的发现极大地丰富了我们对李布晶格的理解,并为基于李布晶格的拓扑态的实验观测提供了指导。