Ke Huang
;
Ajit C. Balram
;
Hailong Fu
;
Chengqi Guo
;
Kenji Watanabe
(National Institute for Materials Science)
;
Takashi Taniguchi
(National Institute for Materials Science)
;
Jainendra K. Jain
;
Jun Zhu
Description:
(abstract)The nature of the many-body state in a Landau level (LL) is crucially dependent on its orbital wave function. For example, in GaAs quantum wells, the half-filled n = 0, 1, and 2 LLs exhibit a metallic, a fractional quantum Hall (FQH), and a charge density wave state, respectively. Multi-component FQH states of electrons with the same orbital wave function but with different spin or valley components, where the interaction is SU(2)-isotropic, have also been observed. Here we report on the observation and theoretical understanding of a new type of “hetero-orbital” two-component FQH states, which occur at the isospin transition of the N = 0 and 1 electron LLs in bilayer graphene. Surprisingly, the underlying SU(2)-anisotropic interaction also stabilizes two- component FQH states and isospin transitions, which however are markedly different from those in homo-orbital systems. We observe a strong two-component 2/5 state, the energy gap of which surpasses its single-component FQH siblings over a wide range of magnetic field before abruptly disappearing at a high field. The anisotropy also leads to a strong asymmetry between parallel- vortex and reverse-vortex composite fermion states. Combined with detailed theoretical calculations, our work contributes new insights into the robustness of multi-component FQH effect.
Rights:
Keyword: fractional quantum Hall (FQH) states , bilayer graphene , hetero-orbital
Date published: 2025-07-22
Publisher: American Physical Society (APS)
Journal:
Funding:
Manuscript type: Publisher's version (Version of record)
MDR DOI:
First published URL: https://doi.org/10.1103/kfn2-qggs
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Updated at: 2026-03-03 08:30:13 +0900
Published on MDR: 2026-03-02 17:20:29 +0900
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