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Gaps induced by inversion symmetry breaking and second-generation Dirac cones in graphene/hexagonal boron nitride

机译:通过倒置对称断裂和石墨烯/六边形氮化硼中的第二代对称锥体引起的间隙

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摘要

Graphene/hexagonal boron nitride (h-BN) has emerged as a model van der Waals heterostructure(1) as the superlattice potential, which is induced by lattice mismatch and crystal orientation, gives rise to various novel quantum phenomena, such as the self-similar Hofstadter butterflystates(2-5). Although the newly generated second-generation Dirac cones (SDCs) are believed to be crucial for understanding such intriguing phenomena, fundamental knowledge of SDCs, such as locations and dispersion, and the effect of inversion symmetry breaking on the gap opening, still remains highly debated due to the lack of direct experimental results. Here we report direct experimental results on the dispersion of SDCs in O degrees-aligned graphene/h-BN heterostructures using angle-resolved photoemission spectroscopy. Our data unambiguously reveal SDCs at the corners of the superlattice Brillouin zone, and at only one of the two superlattice valleys. Moreover, gaps of approximately 100 meV and approximately 160 meV are observed at the SDCs and the original graphene Dirac cone, respectively. Our work highlights the important role of a strong inversion-symmetry-breaking perturbation potential in the physics of graphene/h-BN, and fills critical knowledge gaps in the band structure engineering of Dirac fermions by a superlattice potential.
机译:石墨烯/六边形氮化硼(H-BN)作为模型van der WaaS型异质结构(1)作为超晶格潜力,其被晶格失配和晶体取向引起的,产生了各种新的量子现象,例如自我类似的hofstadter butterflystates(2-5)。虽然新产生的第二代Dirac锥体(SDC)被认为是理解这种有趣现象的至关重要,但SDC的基本知识,例如地点和分散,以及差距开放上的反演对称性的影响仍然高度辩论由于缺乏直接的实验结果。在这里,我们在使用角度分辨的光曝光光谱扫描仪中对SDCS分散的直接实验结果报告了SDCS中的SDC分散。我们的数据明确地揭示了Superlattice Brillouin Zone的角落的SDC,只有两个超薄谷之一。此外,在SDC和原始石墨烯DIRAC锥体上观察到大约100mEV和大约160mEV的间隙。我们的工作突出了强大的反转对称扰动潜力在石墨烯/ H-BN物理学中的重要作用,并通过超晶格潜力填补了Dirac Fermions的带结构工程中的关键知识间隙。

著录项

  • 来源
    《Nature physics》 |2016年第12期|共6页
  • 作者单位

    Tsinghua Univ State Key Lab Low Dimens Quantum Phys Beijing 100084 Peoples R China;

    Chinese Acad Sci Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China;

    Tsinghua Univ State Key Lab Low Dimens Quantum Phys Beijing 100084 Peoples R China;

    Tsinghua Univ State Key Lab Low Dimens Quantum Phys Beijing 100084 Peoples R China;

    Tsinghua Univ State Key Lab Low Dimens Quantum Phys Beijing 100084 Peoples R China;

    Tsinghua Univ State Key Lab Low Dimens Quantum Phys Beijing 100084 Peoples R China;

    Tsinghua Univ State Key Lab Low Dimens Quantum Phys Beijing 100084 Peoples R China;

    Chinese Acad Sci Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China;

    Fudan Univ State Key Lab Surface Phys Shanghai 200433 Peoples R China;

    Fudan Univ State Key Lab Surface Phys Shanghai 200433 Peoples R China;

    Univ Seoul Dept Phys Seoul 02504 South Korea;

    Lawrence Berkeley Natl Lab Adv Light Source Berkeley CA 94720 USA;

    Fudan Univ State Key Lab Surface Phys Shanghai 200433 Peoples R China;

    Chinese Acad Sci Beijing Natl Lab Condensed Matter Phys Beijing 100190 Peoples R China;

    Tsinghua Univ State Key Lab Low Dimens Quantum Phys Beijing 100084 Peoples R China;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 物理学;
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