Premium
Homogeneous 2D MoTe 2 p–n Junctions and CMOS Inverters formed by Atomic‐Layer‐Deposition‐Induced Doping
Author(s) -
Lim June Yeong,
Pezeshki Atiye,
Oh Sehoon,
Kim Jin Sung,
Lee Young Tack,
Yu Sanghyuck,
Hwang Do Kyung,
Lee GwanHyoung,
Choi Hyoung Joon,
Im Seongil
Publication year - 2017
Publication title -
advanced materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 10.707
H-Index - 527
eISSN - 1521-4095
pISSN - 0935-9648
DOI - 10.1002/adma.201701798
Subject(s) - materials science , doping , nanosheet , optoelectronics , dangling bond , cmos , semiconductor , nanotechnology , atomic layer deposition , diode , depletion region , layer (electronics) , silicon
Recently, α‐MoTe 2 , a 2D transition‐metal dichalcogenide (TMD), has shown outstanding properties, aiming at future electronic devices. Such TMD structures without surface dangling bonds make the 2D α‐MoTe 2 a more favorable candidate than conventional 3D Si on the scale of a few nanometers. The bandgap of thin α‐MoTe 2 appears close to that of Si and is quite smaller than those of other typical TMD semiconductors. Even though there have been a few attempts to control the charge‐carrier polarity of MoTe 2 , functional devices such as p–n junction or complementary metal–oxide–semiconductor (CMOS) inverters have not been reported. Here, we demonstrate a 2D CMOS inverter and p–n junction diode in a single α‐MoTe 2 nanosheet by a straightforward selective doping technique. In a single α‐MoTe 2 flake, an initially p‐doped channel is selectively converted to an n‐doped region with high electron mobility of 18 cm 2 V −1 s −1 by atomic‐layer‐deposition‐induced H‐doping. The ultrathin CMOS inverter exhibits a high DC voltage gain of 29, an AC gain of 18 at 1 kHz, and a low static power consumption of a few nanowatts. The results show a great potential of α‐MoTe 2 for future electronic devices based on 2D semiconducting materials.
Accelerating Research
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom
Address
John Eccles HouseRobert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom