Orbitally Controlled Quantum Hall States in Decoupled Two‐Bilayer Graphene Sheets

Abstract The authors report on integer and fractional quantum Hall states in a stack of two twisted Bernal bilayer graphene sheets. By exploiting the momentum mismatch in reciprocal space, the single‐particle tunneling between both bilayers is suppressed. Since the bilayers are spatially separated b...

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Main Authors: Soyun Kim, Dohun Kim, Kenji Watanabe, Takashi Taniguchi, Jurgen H. Smet, Youngwook Kim
Format: Article
Language:English
Published: Wiley 2023-08-01
Series:Advanced Science
Subjects:
Online Access:https://doi.org/10.1002/advs.202300574
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author Soyun Kim
Dohun Kim
Kenji Watanabe
Takashi Taniguchi
Jurgen H. Smet
Youngwook Kim
author_facet Soyun Kim
Dohun Kim
Kenji Watanabe
Takashi Taniguchi
Jurgen H. Smet
Youngwook Kim
author_sort Soyun Kim
collection DOAJ
description Abstract The authors report on integer and fractional quantum Hall states in a stack of two twisted Bernal bilayer graphene sheets. By exploiting the momentum mismatch in reciprocal space, the single‐particle tunneling between both bilayers is suppressed. Since the bilayers are spatially separated by only 0.34 nm, the stack benefits from strong interlayer Coulombic interactions. These interactions can cause the formation of a Bose–Einstein condensate. Indeed, such a condensate is observed for half‐filling in each bilayer sheet. However, only when the partially filled levels have orbital index 1. It is absent for partially filled levels with orbital index 0. This discrepancy is tentatively attributed to the role of skyrmion/anti‐skyrmion pair excitations and the dependence of the energy of these excitations on the orbital index. The application of asymmetric top and bottom gate voltages enables to influence the orbital nature of the electronic states of the graphene bilayers at the chemical potential and to navigate in orbital mixed space. The latter hosts an even denominator fractional quantum Hall state at total filling of −3/2. These observations suggest a unique edge reconstruction involving both electrons and chiral p‐wave composite fermions.
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spelling doaj.art-b4f7452eb3714b0d9af248f8106f81f92023-08-16T02:23:01ZengWileyAdvanced Science2198-38442023-08-011023n/an/a10.1002/advs.202300574Orbitally Controlled Quantum Hall States in Decoupled Two‐Bilayer Graphene SheetsSoyun Kim0Dohun Kim1Kenji Watanabe2Takashi Taniguchi3Jurgen H. Smet4Youngwook Kim5Department of Physics and Chemistry Daegu Gyeongbuk Institute of Science and Technology (DGIST) Daegu 42988 Republic of KoreaDepartment of Physics and Chemistry Daegu Gyeongbuk Institute of Science and Technology (DGIST) Daegu 42988 Republic of KoreaResearch Center for Functional Materials National Institute for Materials Science Tsukuba 305‐0044 JapanInternational Center for Materials Nanoarchitectonics National Institute for Materials Science Tsukuba 305‐0044 JapanMax Planck Institute for Solid State Research 70569 Stuttgart GermanyDepartment of Physics and Chemistry Daegu Gyeongbuk Institute of Science and Technology (DGIST) Daegu 42988 Republic of KoreaAbstract The authors report on integer and fractional quantum Hall states in a stack of two twisted Bernal bilayer graphene sheets. By exploiting the momentum mismatch in reciprocal space, the single‐particle tunneling between both bilayers is suppressed. Since the bilayers are spatially separated by only 0.34 nm, the stack benefits from strong interlayer Coulombic interactions. These interactions can cause the formation of a Bose–Einstein condensate. Indeed, such a condensate is observed for half‐filling in each bilayer sheet. However, only when the partially filled levels have orbital index 1. It is absent for partially filled levels with orbital index 0. This discrepancy is tentatively attributed to the role of skyrmion/anti‐skyrmion pair excitations and the dependence of the energy of these excitations on the orbital index. The application of asymmetric top and bottom gate voltages enables to influence the orbital nature of the electronic states of the graphene bilayers at the chemical potential and to navigate in orbital mixed space. The latter hosts an even denominator fractional quantum Hall state at total filling of −3/2. These observations suggest a unique edge reconstruction involving both electrons and chiral p‐wave composite fermions.https://doi.org/10.1002/advs.202300574Bose–Einstein condensationfractional quantum Hall effectquantum Hall effecttwisted double bilayer graphene
spellingShingle Soyun Kim
Dohun Kim
Kenji Watanabe
Takashi Taniguchi
Jurgen H. Smet
Youngwook Kim
Orbitally Controlled Quantum Hall States in Decoupled Two‐Bilayer Graphene Sheets
Advanced Science
Bose–Einstein condensation
fractional quantum Hall effect
quantum Hall effect
twisted double bilayer graphene
title Orbitally Controlled Quantum Hall States in Decoupled Two‐Bilayer Graphene Sheets
title_full Orbitally Controlled Quantum Hall States in Decoupled Two‐Bilayer Graphene Sheets
title_fullStr Orbitally Controlled Quantum Hall States in Decoupled Two‐Bilayer Graphene Sheets
title_full_unstemmed Orbitally Controlled Quantum Hall States in Decoupled Two‐Bilayer Graphene Sheets
title_short Orbitally Controlled Quantum Hall States in Decoupled Two‐Bilayer Graphene Sheets
title_sort orbitally controlled quantum hall states in decoupled two bilayer graphene sheets
topic Bose–Einstein condensation
fractional quantum Hall effect
quantum Hall effect
twisted double bilayer graphene
url https://doi.org/10.1002/advs.202300574
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