Author
Listed:
- Hongyuan Li
(University of California at Berkeley
University of California at Berkeley
Lawrence Berkeley National Laboratory)
- Ziyu Xiang
(University of California at Berkeley
University of California at Berkeley
Lawrence Berkeley National Laboratory)
- Tianle Wang
(University of California at Berkeley
Lawrence Berkeley National Laboratory)
- Mit H. Naik
(University of California at Berkeley
Lawrence Berkeley National Laboratory)
- Woochang Kim
(University of California at Berkeley
Lawrence Berkeley National Laboratory)
- Jiahui Nie
(University of California at Berkeley)
- Shiyu Li
(University of California at Berkeley)
- Zhehao Ge
(University of California at Berkeley)
- Zehao He
(University of California at Berkeley)
- Yunbo Ou
(Arizona State University)
- Rounak Banerjee
(Arizona State University)
- Takashi Taniguchi
(National Institute for Materials Science)
- Kenji Watanabe
(National Institute for Materials Science)
- Sefaattin Tongay
(Arizona State University)
- Alex Zettl
(University of California at Berkeley
Lawrence Berkeley National Laboratory
Kavli Energy Nano Sciences Institute at the University of California Berkeley and the Lawrence Berkeley National Laboratory)
- Steven G. Louie
(University of California at Berkeley
Lawrence Berkeley National Laboratory)
- Michael P. Zaletel
(University of California at Berkeley)
- Michael F. Crommie
(University of California at Berkeley
Lawrence Berkeley National Laboratory
Kavli Energy Nano Sciences Institute at the University of California Berkeley and the Lawrence Berkeley National Laboratory)
- Feng Wang
(University of California at Berkeley
Lawrence Berkeley National Laboratory
Kavli Energy Nano Sciences Institute at the University of California Berkeley and the Lawrence Berkeley National Laboratory)
Abstract
One-dimensional (1D) interacting electrons are often described as a Luttinger liquid1–4 having properties that are intrinsically different from those of Fermi liquids in higher dimensions5,6. In materials systems, 1D electrons exhibit exotic quantum phenomena that can be tuned by both intra- and inter-1D-chain electronic interactions, but their experimental characterization can be challenging. Here we demonstrate that layer-stacking domain walls (DWs) in van der Waals heterostructures form a broadly tunable Luttinger liquid system, including both isolated and coupled arrays. We have imaged the evolution of DW Luttinger liquids under different interaction regimes tuned by electron density using scanning tunnelling microscopy. Single DWs at low carrier density are highly susceptible to Wigner crystallization consistent with a spin-incoherent Luttinger liquid, whereas at intermediate densities dimerized Wigner crystals form because of an enhanced magneto-elastic coupling. Periodic arrays of DWs exhibit an interplay between intra- and inter-chain interactions that gives rise to new quantum phases. At low electron densities, inter-chain interactions are dominant and induce a 2D electron crystal composed of phased-locked 1D Wigner crystal in a staggered configuration. Increased electron density causes intra-chain fluctuation potentials to dominate, leading to an electronic smectic liquid crystal phase in which electrons are ordered with algebraical correlation decay along the chain direction but disordered between chains. Our work shows that layer-stacking DWs in 2D heterostructures provides opportunities to explore Luttinger liquid physics.
Suggested Citation
Hongyuan Li & Ziyu Xiang & Tianle Wang & Mit H. Naik & Woochang Kim & Jiahui Nie & Shiyu Li & Zhehao Ge & Zehao He & Yunbo Ou & Rounak Banerjee & Takashi Taniguchi & Kenji Watanabe & Sefaattin Tongay , 2024.
"Imaging tunable Luttinger liquid systems in van der Waals heterostructures,"
Nature, Nature, vol. 631(8022), pages 765-770, July.
Handle:
RePEc:nat:nature:v:631:y:2024:i:8022:d:10.1038_s41586-024-07596-6
DOI: 10.1038/s41586-024-07596-6
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