Volume 5, Issue 10
Communication

Gate‐Tunable Electrical Transport in Thin 2M‐WS2 Flakes

Xiangli Che

State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, 200050 P. R. China

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Yujun Deng

State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, 200438 P. R. China

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Yuqiang Fang

State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, 200050 P. R. China

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Jie Pan

State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, 200050 P. R. China

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Yijun Yu

State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai, 200438 P. R. China

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Fuqiang Huang

Corresponding Author

E-mail address: huagnfq@mail.sic.ac.cn

State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, 200050 P. R. China

State Key Laboratory of Rare Earth Materials Chemistry and Applications, College of Chemistry and Molecular Engineering, Peking University, Beijing, 100871 P. R. China

E‐mail: huagnfq@mail.sic.ac.cnSearch for more papers by this author
First published: 23 July 2019

Abstract

Electrolyte gating has been employed as an effective way to modulate the electronic properties of transition metal dichalcogenides (TMDs) by carrier doping over a wide range. Here, the carrier density of a new metastable phase of TMD material 2M‐WS2 is controlled by electrolyte gating to achieve reversible transitions between the superconducting state, metallic state, and insulating state. Pristine 2M‐WS2 has a superconducting transition temperature (T c) of 8.9 K with a hole‐type carrier density of 9.05 × 1021 cm−3 at 100 K. A gate voltage (V g) is applied between the sample and a side gate, which are both immersed in a droplet of gel‐like Li‐ion electrolyte (LiClO4 dissolved in polyethylene oxide matrix). When V g = −3.5 V, the sample is in its pristine superconducting phase. With increasing V g, the lithium ions gradually intercalate into the layered sample and tune it from a superconductor to an insulator. By precise tuning of V g in this device, the entire phase diagram of 2M‐WS2 over a large range of carrier density is obtained.

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