Quantum Phase Transitions in Graphene Coupled to a Twisted WSe <sub>2</sub> Moiré Ferroelectricity
Article 2025 en
Authors
BS
Budhi Singh
YH
Yasir Hassan
NA
Nasir Ali
Abstract
1 min read
Sublattice symmetry in graphene governs its Dirac semimetal behavior, where electrons exhibit linear dispersion, limiting its potential for technological applications. Here, moiré ferroelectricity in twisted WSe<sub>2</sub> (t-WSe<sub>2</sub>) is exploited to break graphene's sublattice symmetry, inducing a metal-to-insulator transition (MIT) near room temperature. The periodic polarization domains in t-WSe<sub>2</sub> imprint an electrostatic potential onto graphene, breaking its sublattice symmetry and leading to the emergence of a local Dirac point, as observed in the transfer characteristics of a t-WSe<sub>2</sub>/graphene field-effect transistor. Temperature-dependent transport measurements reveal multiple MIT points at relatively high temperatures, attributed to the room-temperature ferroelectric polarization in t-WSe<sub>2</sub>. Furthermore, A distinct metallic phases is identified exhibiting T<sup>2</sup> and linear-T dependent longitudinal resistance under electrostatic doping, indicative of Fermi-liquid and non-Fermi-liquid metallic behavior, respectively. Finally, finite-size scaling analysis of R<sub>xx</sub> near the MIT points indicates continuous quantum phase transitions near room temperature, establishing moiré ferroelectricity as a pathway for engineering quantum electronic phases of monolayer graphene at ambient conditions.
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