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arXiv 1801.07550cond-mat.mtrl-scicond-mat.str-elphysics.comp-ph
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Kagome石墨烯及其相关结构的铁磁性和Wigner结晶

Ferromagnetism and Wigner crystallization in Kagome graphene and related structures

Yuanping Chen, Shenglong Xu, Yuee Xie, Chengyong Zhong, Congjun Wu, S. B. Zhang

摘要:

由于态密度的发散,平带中的相互作用被放大,这引起了各种多体现象,如铁磁性和维格纳结晶。然而,到目前为止,平带物理的研究大多是建立在模型系统的基础上,使其实验实现成为一个遥远的未来。在这里,我们提出了一类由真实原子组成的系统,即具有现实物理相互作用的碳原子(在这里称为Kagome graphene/graphyne)。密度泛函理论计算表明,这些Kagome晶格提供了一种可控的方式来实现足够接近费米能级的鲁棒平坦带。在空穴掺杂时,它们分裂成不同能量的自旋极化带,导致平带铁磁性。在半填充时,这种分裂达到768 meV的最高水平。对于较小的填充物,例如,另一方面,当ν=1/6时,自发地形成维格纳晶体,其中电子形成位于规则三角形晶格的网格点上的闭合环。它打破了原来的可果美晶格的平移对称性。我们进一步表明,Kagome晶格表现出良好的机械稳定性,在此基础上,Kagome石墨烯的实验实现的可能途径也提出了。

英文摘要:

Interaction in a flat band is magnified due to the divergence in the density of states, which gives rise to a variety of many-body phenomena such as ferromagnetism and Wigner crystallization. Until now, however, most studies of the flat band physics are based on model systems, making their experimental realization a distant future. Here, we propose a class of systems made of real atoms, namely, carbon atoms with realistic physical interactions (dubbed here as Kagome graphene/graphyne). Density functional theory calculations reveal that these Kagome lattices offer a controllable way to realize robust flat bands sufficiently close to the Fermi level. Upon hole doping, they split into spin-polarized bands at different energies to result in a flat-band ferromagnetism. At a half filling, this splitting reaches its highest level of 768 meV. At smaller fillings, e.g., when ν=1/6, on the other hand, a Wigner crystal spontaneously forms, where the electrons form closed loops localized on the grid points of a regular triangular lattice. It breaks the translational symmetry of the original Kagome lattice. We further show that the Kagome lattices exhibit good mechanical stabilities, based on which a possible route for experimental realization of the Kagome graphene is also proposed.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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