论文标题

在压力下,魔法角扭曲的双层石墨烯中的栅极可调铁磁性的第一原理计算

First-principles calculation of gate-tunable ferromagnetism in magic-angle twisted bilayer graphene under pressure

论文作者

Chen, Xiao, Liu, Shuanglong, Fry, James N, Cheng, Hai-Ping

论文摘要

魔法角扭曲的双层石墨烯(MATBG)是一个高度可调的平台,用于研究密切相关的现象,例如高$ t_c $超导性和量子自旋液体,这是由于通过对兴趣水平的易于控制和敏感的依赖性依赖魔术角度对静态角度的依赖。 MATBG中相关的绝缘状态,非常规的超导性和铁磁性的实验观察表明,该系统表现出丰富的外来阶段。在这项工作中,使用密度功能理论的计算与有效筛选介质方法结合使用,我们在压力下以$ 2.88 \ unicode {xb0} $的扭曲角度找到MATBG,并模拟其电子状态在掺杂水平和平面电场外电场时如何演变。我们的计算表明,在两个电子和每个Moiré单位细胞之间的掺杂水平下,在AA堆叠位点旋转密度的铁磁溶液的能量低于非磁性溶液。这种铁磁状态的磁矩随着电子和四个电子/孔掺杂的每个moiré单位电池而消失的电子和孔掺杂,并消失。在有限的掺杂时,可以在费米级和周围的分散带之间的平坦带和周围的分散带之间进行杂交。此外,在零掺杂时增加平面外电场后,可以看到从铁磁状态到非磁性的过渡。我们还通过Wannier函数分析了由于平坦的频带而分析层间键合特征。最后,我们报告了在特定掺杂水平的铁磁状态下平面带的微不足道的带拓扑。

Magic-angle twisted bilayer graphene (MATBG) is notable as a highly tunable platform for investigating strongly correlated phenomena such as high-$T_c$ superconductivity and quantum spin liquids, due to easy control of doping level through gating and sensitive dependence of the magic angle on hydrostatic pressure. Experimental observations of correlated insulating states, unconventional superconductivity and ferromagnetism in MATBG indicate that this system exhibits rich exotic phases. In this work, using density functional theory calculations in conjunction with the effective screening medium method, we find the MATBG under pressure at a twisting angle of $2.88\unicode{xb0}$ and simulate how its electronic states evolve when doping level and out-of-plane electric field are gate-tuned. Our calculations show that, at doping levels between two electrons and four holes per moiré unit cell, a ferromagnetic solution with spin density localized at AA stacking sites is lower in energy than the nonmagnetic solution. The magnetic moment of this ferromagnetic state decreases with both electron and hole doping and vanishes at four electrons/holes doped per moiré unit cell. Hybridization between the flat bands at the Fermi level and the surrounding dispersive bands can take place at finite doping. Moreover, upon increasing the out-of-plane electric field at zero doping, a transition from the ferromagnetic state to the nonmagnetic one is seen. We also analyze the interlayer bonding character due to the flat bands via Wannier functions. Finally, we report trivial band topology of the flat bands in the ferromagnetic state at a certain doping level.

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