Surface-Shielding Nanostructures Derived from Self-Assembled Block Copolymers Enable Reliable Plasma Doping for Few-Layer Transition Metal Dichalcogenides

被引:20
作者
Yim, Soonmin [1 ]
Sim, Dong Min [1 ]
Park, Woon Ik [2 ]
Choi, Min-Jae [1 ]
Choi, Jaesuk [1 ]
Jeon, Jaebeom [1 ]
Kim, Kwang Ho [2 ,3 ]
Jung, Yeon Sik [1 ]
机构
[1] Korea Adv Inst Sci & Technol, Dept Mat Sci & Engn, 291 Daehak Ro, Daejeon 305701, South Korea
[2] Global Frontier R&D Ctr Hybrid Interface Mat HIM, Busandaehak Ro 63Beon Gil, Busan 609735, South Korea
[3] Pusan Natl Univ, Sch Mat Sci & Engn, Busandaehak Ro 63 Beon Gil, Busan 609735, South Korea
基金
新加坡国家研究基金会;
关键词
block copolymer; molybdenum disulfide; plasma doping; self-assembly; transition metal dichalcogenide; FIELD-EFFECT TRANSISTORS; LARGE-AREA; MOS2; GRAPHENE; MONOLAYER; PHOTOLUMINESCENCE; TRANSPARENT; STOICHIOMETRY; GRAPHOEPITAXY; ELECTRONICS;
D O I
10.1002/adfm.201600654
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
Precise modulation of electrical and optical properties of 2D transition metal dichalcogenides (TMDs) is required for their application to high-performance devices. Although conventional plasma-based doping methods have provided excellent controllability and reproducibility for bulk or relatively thick TMDs, the application of plasma doping for ultrathin few-layer TMDs has been hindered by serious degradation of their properties. Herein, a reliable and universal doping route is reported for few-layer TMDs by employing surface-shielding nanostructures during a plasma-doping process. It is shown that the surface-protection oxidized polydimethylsiloxane nanostructures obtained from the sub-20 nm self-assembly of Si-containing block copolymers can preserve the integrity of 2D TMDs and maintain high mobility while affording extensive control over the doping level. For example, the self-assembled nanostructures form periodically arranged plasma-blocking and plasma-accepting nanoscale regions for realizing modulated plasma doping on few-layer MoS2, controlling the n-doping level of few-layer MoS2 from 1.9 x 10(11) cm(-2) to 8.1 x 10(11) cm(-2) via the local generation of extra sulfur vacancies without compromising the carrier mobility.
引用
收藏
页码:5631 / 5640
页数:10
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