2022
DOI: 10.1038/s41565-022-01248-4
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Quantum Hall phase in graphene engineered by interfacial charge coupling

Abstract: The quantum Hall effect can be substantially affected by interfacial coupling between the host two-dimensional electron gases and the substrate, and has been predicted to give rise to exotic topological states. Yet the understanding of the underlying physics and the controllable engineering of this interaction remains challenging. Here we demonstrate the observation of an unusual quantum Hall effect, which differs markedly from that of the known picture, in graphene samples in contact with an antiferromagnetic… Show more

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Cited by 31 publications
(35 citation statements)
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References 49 publications
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“…2(d). This perfectly explains the recent experiment in gate-controlled graphene-CrOCl heterostructure, in which the Fermi velocity around CNP is significantly enhanced compared to noninteracting value at slight carrier doping, such that robust quantum Hall effect can be observed under tiny vertical magnetic fields (∼ 0.1 T) and high temperatures [19]. We note that the EC state may be stabilized by vertical magnetic fields even when the carrier density in the substrate exceeds the zero-field threshold value [43,44], which in turn boosts the low-field, high-temperature quantum Hall effect in the graphene layer due to the scenario discussed above.…”
Section: Coulomb Interactions In Graphenesupporting
confidence: 87%
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“…2(d). This perfectly explains the recent experiment in gate-controlled graphene-CrOCl heterostructure, in which the Fermi velocity around CNP is significantly enhanced compared to noninteracting value at slight carrier doping, such that robust quantum Hall effect can be observed under tiny vertical magnetic fields (∼ 0.1 T) and high temperatures [19]. We note that the EC state may be stabilized by vertical magnetic fields even when the carrier density in the substrate exceeds the zero-field threshold value [43,44], which in turn boosts the low-field, high-temperature quantum Hall effect in the graphene layer due to the scenario discussed above.…”
Section: Coulomb Interactions In Graphenesupporting
confidence: 87%
“…Especially, how the mutual couplings would affect the interacting electronic states in both systems. Inspired by recent pioneering experiments in CrOCl-graphene [19], 1T-TaS 2 -graphene [20], and CrI 3 -graphene [21] heterostructures, here we propose that such a scenario (of interacting Dirac fermions coupled with the correlated electrons in charge doped TMO/TMC insulators) can be realized in graphene-insulator heterostructures with gate tunable band alignment. In this work, we show that, by virtue of the interlayer Coulomb coupling between the interacting electrons in the two layers, intriguing correlated physics that cannot be seen in either individual layer would emerge in a cooperative and synergistic manner in such band-aligned graphene-insulator heterostructures.…”
Section: Introductionmentioning
confidence: 95%
“…最后, 本综述将讨论一类新型石墨烯异 质结体系: 能带对齐的石墨烯和绝缘衬底形成的异 质结体系中的新奇物理. 通过门电压调控的电荷转 移, 在绝缘衬底上的载流子由于长程库仑作用可以 形成长程电荷序, 并与石墨烯中的狄拉克费米子耦 合, 进而降低狄拉克电子的非相互作用费米速度 [86] , 让电子间库仑相互作用效应更加显著, 衍生出新的 关联拓扑物态 [86,87] . (d)魔角双层石墨烯的能带.…”
Section: 而在各类转角多层石墨烯体系中 平带在半填充时unclassified
“…(a) Flat bands of magic-angle TBG with the octupolar-type phonon modes under frozen mode approximation [85] ; (b) increasing bandgap as a function of average displacement amplitudes [85] ; (c) strength of electron-phonon coupling verse Fermi level in the magic-angle TBG [85] ; (d) charge order with the quadrupolar-type phonon modes under frozen mode approximation [85] . Lu等 [86] 和Wang等 [87] 指出, 如果将石墨烯 放置于具有长程电荷序的绝缘衬底之上, 会构成一 种新型二维材料异质结体系(见图9(a)). 长程电荷 序的形成本身也依赖于强电子间库仑相互作用, 如 低浓度的二维电子气在长程库仑作用的驱动下会 进入到维格纳晶体态 [187][188][189] 为衬底的单层石墨烯器件中实现 [87,190,191] .…”
Section: 魔角双层石墨烯的电声耦合效应mentioning
confidence: 99%
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