| Literature DB >> 35508779 |
Pengjie Wang1, Guo Yu1,2, Yves H Kwan3, Yanyu Jia1, Shiming Lei4,5, Sebastian Klemenz4,6, F Alexandre Cevallos4, Ratnadwip Singha4, Trithep Devakul7, Kenji Watanabe8, Takashi Taniguchi9, Shivaji L Sondhi1,3, Robert J Cava4, Leslie M Schoop4, Siddharth A Parameswaran3, Sanfeng Wu10.
Abstract
The Luttinger liquid (LL) model of one-dimensional (1D) electronic systems provides a powerful tool for understanding strongly correlated physics, including phenomena such as spin-charge separation1. Substantial theoretical efforts have attempted to extend the LL phenomenology to two dimensions, especially in models of closely packed arrays of 1D quantum wires2-13, each being described as a LL. Such coupled-wire models have been successfully used to construct two-dimensional (2D) anisotropic non-Fermi liquids2-6, quantum Hall states7-9, topological phases10,11 and quantum spin liquids12,13. However, an experimental demonstration of high-quality arrays of 1D LLs suitable for realizing these models remains absent. Here we report the experimental realization of 2D arrays of 1D LLs with crystalline quality in a moiré superlattice made of twisted bilayer tungsten ditelluride (tWTe2). Originating from the anisotropic lattice of the monolayer, the moiré pattern of tWTe2 hosts identical, parallel 1D electronic channels, separated by a fixed nanoscale distance, which is tuneable by the interlayer twist angle. At a twist angle of approximately 5 degrees, we find that hole-doped tWTe2 exhibits exceptionally large transport anisotropy with a resistance ratio of around 1,000 between two orthogonal in-plane directions. The across-wire conductance exhibits power-law scaling behaviours, consistent with the formation of a 2D anisotropic phase that resembles an array of LLs. Our results open the door for realizing a variety of correlated and topological quantum phases based on coupled-wire models and LL physics.Entities:
Year: 2022 PMID: 35508779 DOI: 10.1038/s41586-022-04514-6
Source DB: PubMed Journal: Nature ISSN: 0028-0836 Impact factor: 49.962