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Correlated insulator in the kagome flat band of a two-dimensional electrostatic crystal. / Wang, Daisy Q.; Krix, Zeb; Tkachenko, Olga A. et al.

In: Nature Physics, Vol. 22, 07.2026, p. 1079–1086.

Research output: Contribution to journalArticlepeer-review

Harvard

Wang, DQ, Krix, Z, Tkachenko, OA, Tkachenko, VA, Chen, C, Farrer, I, Ritchie, DA, Sushkov, OP, Hamilton, AR & Klochan, O 2026, 'Correlated insulator in the kagome flat band of a two-dimensional electrostatic crystal', Nature Physics, vol. 22, pp. 1079–1086. https://doi.org/10.1038/s41567-026-03291-7

APA

Wang, D. Q., Krix, Z., Tkachenko, O. A., Tkachenko, V. A., Chen, C., Farrer, I., Ritchie, D. A., Sushkov, O. P., Hamilton, A. R., & Klochan, O. (2026). Correlated insulator in the kagome flat band of a two-dimensional electrostatic crystal. Nature Physics, 22, 1079–1086. https://doi.org/10.1038/s41567-026-03291-7

Vancouver

Wang DQ, Krix Z, Tkachenko OA, Tkachenko VA, Chen C, Farrer I et al. Correlated insulator in the kagome flat band of a two-dimensional electrostatic crystal. Nature Physics. 2026 Jul;22:1079–1086. doi: 10.1038/s41567-026-03291-7

Author

Wang, Daisy Q. ; Krix, Zeb ; Tkachenko, Olga A. et al. / Correlated insulator in the kagome flat band of a two-dimensional electrostatic crystal. In: Nature Physics. 2026 ; Vol. 22. pp. 1079–1086.

BibTeX

@article{a6fe7ef81602462baf7687073de99ad3,
title = "Correlated insulator in the kagome flat band of a two-dimensional electrostatic crystal",
abstract = "The electronic properties of solids are determined by their crystal structure and electron interactions, giving rise to phenomena such as superconductivity, strange metals and correlated insulators. Many of these effects remain poorly understood, motivating efforts to create artificial crystals that mimic real materials while allowing controlled tuning of key parameters. Cold atoms in optical lattices offer flexibility but cannot reproduce the long-range Coulomb interactions and hopping present in solids. Solid-state systems naturally support these features, although they suffer from tunability and flexibility issues. Here we demonstrate a highly tunable artificial crystal formed by superimposing a periodic electrostatic potential onto a two-dimensional electron gas in a shallow GaAs quantum well. This engineered lattice exhibits a band structure characteristic of the artificial triangular lattice, distinct from that of the underlying cubic crystal. Electronic transport measurements show a sign change in the Hall coefficient as the chemical potential sweeps through the artificial bands. The band structure can be continuously tuned to realize linear graphene-like and flat kagome-like bands within a single device. A strong insulating state emerges at half filling of the kagome flat band, consistent with interaction-driven behaviour. This tunability provides an opportunity to explore correlated quantum states in a controlled setting.",
author = "Wang, {Daisy Q.} and Zeb Krix and Tkachenko, {Olga A.} and Tkachenko, {Vitaly A.} and Chong Chen and Ian Farrer and Ritchie, {David A.} and Sushkov, {Oleg P.} and Hamilton, {Alexander R.} and Oleh Klochan",
note = "Open access funding provided through UNSW Library.",
year = "2026",
month = jul,
doi = "10.1038/s41567-026-03291-7",
language = "English",
volume = "22",
pages = "1079–1086",
journal = "Nature Physics",
issn = "1745-2473",
publisher = "Nature Publishing Group",

}

RIS

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T1 - Correlated insulator in the kagome flat band of a two-dimensional electrostatic crystal

AU - Wang, Daisy Q.

AU - Krix, Zeb

AU - Tkachenko, Olga A.

AU - Tkachenko, Vitaly A.

AU - Chen, Chong

AU - Farrer, Ian

AU - Ritchie, David A.

AU - Sushkov, Oleg P.

AU - Hamilton, Alexander R.

AU - Klochan, Oleh

N1 - Open access funding provided through UNSW Library.

PY - 2026/7

Y1 - 2026/7

N2 - The electronic properties of solids are determined by their crystal structure and electron interactions, giving rise to phenomena such as superconductivity, strange metals and correlated insulators. Many of these effects remain poorly understood, motivating efforts to create artificial crystals that mimic real materials while allowing controlled tuning of key parameters. Cold atoms in optical lattices offer flexibility but cannot reproduce the long-range Coulomb interactions and hopping present in solids. Solid-state systems naturally support these features, although they suffer from tunability and flexibility issues. Here we demonstrate a highly tunable artificial crystal formed by superimposing a periodic electrostatic potential onto a two-dimensional electron gas in a shallow GaAs quantum well. This engineered lattice exhibits a band structure characteristic of the artificial triangular lattice, distinct from that of the underlying cubic crystal. Electronic transport measurements show a sign change in the Hall coefficient as the chemical potential sweeps through the artificial bands. The band structure can be continuously tuned to realize linear graphene-like and flat kagome-like bands within a single device. A strong insulating state emerges at half filling of the kagome flat band, consistent with interaction-driven behaviour. This tunability provides an opportunity to explore correlated quantum states in a controlled setting.

AB - The electronic properties of solids are determined by their crystal structure and electron interactions, giving rise to phenomena such as superconductivity, strange metals and correlated insulators. Many of these effects remain poorly understood, motivating efforts to create artificial crystals that mimic real materials while allowing controlled tuning of key parameters. Cold atoms in optical lattices offer flexibility but cannot reproduce the long-range Coulomb interactions and hopping present in solids. Solid-state systems naturally support these features, although they suffer from tunability and flexibility issues. Here we demonstrate a highly tunable artificial crystal formed by superimposing a periodic electrostatic potential onto a two-dimensional electron gas in a shallow GaAs quantum well. This engineered lattice exhibits a band structure characteristic of the artificial triangular lattice, distinct from that of the underlying cubic crystal. Electronic transport measurements show a sign change in the Hall coefficient as the chemical potential sweeps through the artificial bands. The band structure can be continuously tuned to realize linear graphene-like and flat kagome-like bands within a single device. A strong insulating state emerges at half filling of the kagome flat band, consistent with interaction-driven behaviour. This tunability provides an opportunity to explore correlated quantum states in a controlled setting.

UR - https://www.scopus.com/pages/publications/105038401679

UR - https://www.mendeley.com/catalogue/4dd9afc5-4952-37e5-8b11-21eb8f7d4a0a/

U2 - 10.1038/s41567-026-03291-7

DO - 10.1038/s41567-026-03291-7

M3 - Article

C2 - 42539552

VL - 22

SP - 1079

EP - 1086

JO - Nature Physics

JF - Nature Physics

SN - 1745-2473

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