<p>Recently, multilayer graphene systems have attracted significant attention due to the discovery of many intriguing phases, particularly quantum anomalous Hall (QAH) states. In rhombohedral pentalayer graphene, QAH states with Chern numbers <i>C</i>&#xa0;=&#xa0;−&#xa0;5 and <i>C</i>&#xa0;=&#xa0;−&#xa0;3 have been observed, but the origin of the <i>C</i>&#xa0;=&#xa0;−&#xa0;3 state remains unclear. Here we show that trigonal warping, staggered layer order, and displacement field together generate an asynchronous mass inversion mechanism. Trigonal warping splits the low-energy bands into one central touching point and three satellite Dirac cones, while the coexistence of staggered layer order and displacement field produces a momentum-dependent mass term. In rhombohedral pentalayer graphene, as the displacement field increases, mass inversion occurs first at the satellite cones and then at the central touching point, yielding the <i>C</i>&#xa0;=&#xa0;−&#xa0;3 state and the subsequent transition to <i>C</i>&#xa0;=&#xa0;−&#xa0;5. This mechanism also explains the observed <i>C</i>&#xa0;=&#xa0;6 state in Bernal-stacked tetralayer graphene, guiding future experiments to engineer tunable high-Chern phases.</p><p></p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Quantum anomalous Hall states enriched by asynchronous mass inversion in multilayer graphene

  • Xilin Feng,
  • Zi-Ting Sun,
  • K. T. Law

摘要

Recently, multilayer graphene systems have attracted significant attention due to the discovery of many intriguing phases, particularly quantum anomalous Hall (QAH) states. In rhombohedral pentalayer graphene, QAH states with Chern numbers C = − 5 and C = − 3 have been observed, but the origin of the C = − 3 state remains unclear. Here we show that trigonal warping, staggered layer order, and displacement field together generate an asynchronous mass inversion mechanism. Trigonal warping splits the low-energy bands into one central touching point and three satellite Dirac cones, while the coexistence of staggered layer order and displacement field produces a momentum-dependent mass term. In rhombohedral pentalayer graphene, as the displacement field increases, mass inversion occurs first at the satellite cones and then at the central touching point, yielding the C = − 3 state and the subsequent transition to C = − 5. This mechanism also explains the observed C = 6 state in Bernal-stacked tetralayer graphene, guiding future experiments to engineer tunable high-Chern phases.