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Strong Piezoelectricity in 3R‐MoS<sub>2</sub> Flakes

Hamida HallilCentre of Micro‐/Nanoelectronics (CMNE) School of Electrical and Electronic Engineering Nanyang Technological University Singapore 639798 SingaporeWeifan CaiCentre of Micro‐/Nanoelectronics (CMNE) School of Electrical and Electronic Engineering Nanyang Technological University Singapore 639798 SingaporeKang ZhangCentre of Micro‐/Nanoelectronics (CMNE) School of Electrical and Electronic Engineering Nanyang Technological University Singapore 639798 SingaporePeng YuSchool of Materials Science and Engineering Sun Yat‐sen University Guangzhou Guangdong 510275 ChinaSheng LiuDivision of Physics and Applied Physics School of Physical and Mathematical Sciences Nanyang Technological University Singapore 637371 SingaporeRan XuCentre of Micro‐/Nanoelectronics (CMNE) School of Electrical and Electronic Engineering Nanyang Technological University Singapore 639798 SingaporeChao ZhuSchool of Materials Science &amp; Engineering Nanyang Technological University Singapore 639798 SingaporeQihua XiongDivision of Physics and Applied Physics School of Physical and Mathematical Sciences Nanyang Technological University Singapore 637371 SingaporeZheng LiuCentre of Micro‐/Nanoelectronics (CMNE) School of Electrical and Electronic Engineering Nanyang Technological University Singapore 639798 SingaporeQing ZhangCentre of Micro‐/Nanoelectronics (CMNE) School of Electrical and Electronic Engineering Nanyang Technological University Singapore 639798 Singapore
2022en
ABI

Abstract

Abstract Distinct from conventional 2H‐MoS 2 , recently synthesized 3R‐MoS 2 exhibits a noncentrosymmetric atomic structure of the trigonal “building blocks” and, thus, remarkable piezoelectric characteristics of ultrathin 3R‐MoS 2 flakes are predicated theoretically. This paper reveals, for the first time, very high piezoelectricity in 3R‐MoS 2 flakes experimentally. Through applying mechanical stress to a 48 nm 3R‐MoS 2 flake, a high output power density of 65 mW m ‐2 is obtained and is at least one order larger than those from the corresponding monolayer MoS 2 flake. With out‐of‐plane lateral piezoresponse force microscopy technique, the two piezoelectric coefficients d 33 and d 13 are analyzed to be ≈0.9 and ≈1.6 pm V ‐1 , respectively. These piezoelectric coefficients are not apparently dependent on the flake thickness. The findings suggest that 3R‐MoS 2 is of excellent piezoelectric properties and it can be an excellent material for novel piezoelectric devices.

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