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Homogeneous 2D MoTe<sub>2</sub> p–n Junctions and CMOS Inverters formed by Atomic‐Layer‐Deposition‐Induced Doping

June Yeong LimInstitute of Physics and Applied Physics Yonsei University 50 Yonsei‐ro Seodaemun‐gu Seoul 03722 South KoreaAtiye PezeshkiInstitute of Physics and Applied Physics Yonsei University 50 Yonsei‐ro Seodaemun‐gu Seoul 03722 South KoreaSehoon OhInstitute of Physics and Applied Physics Yonsei University 50 Yonsei‐ro Seodaemun‐gu Seoul 03722 South KoreaJin Sung KimInstitute of Physics and Applied Physics Yonsei University 50 Yonsei‐ro Seodaemun‐gu Seoul 03722 South KoreaYoung Tack LeeCenter for Optoelectronic Materials and Devices Post‐Silicon Semiconductor Institute Korea Institute of Science and Technology (KIST) Hwarangno 14 gil 5 Seongbuk‐gu Seoul 02792 South KoreaSanghyuck YuInstitute of Physics and Applied Physics Yonsei University 50 Yonsei‐ro Seodaemun‐gu Seoul 03722 South KoreaDo Kyung HwangCenter for Optoelectronic Materials and Devices Post‐Silicon Semiconductor Institute Korea Institute of Science and Technology (KIST) Hwarangno 14 gil 5 Seongbuk‐gu Seoul 02792 South KoreaGwan‐Hyoung LeeDepartment of Materials Science and Engineering Yonsei University Seoul 03722 South KoreaHyoung Joon ChoiInstitute of Physics and Applied Physics Yonsei University 50 Yonsei‐ro Seodaemun‐gu Seoul 03722 South KoreaSeongil ImInstitute of Physics and Applied Physics Yonsei University 50 Yonsei‐ro Seodaemun‐gu Seoul 03722 South Korea
2017en
ABI

Аннотация

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.

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