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Conversion of Charge Carrier Polarity in MoTe(2) Field Effect Transistor via Laser Doping
A two-dimensional (2D) atomic crystalline transition metal dichalcogenides has shown immense features, aiming for future nanoelectronic devices comparable to conventional silicon (Si). 2D molybdenum ditelluride (MoTe(2)) has a small bandgap, appears close to that of Si, and is more favorable than ot...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10222443/ https://www.ncbi.nlm.nih.gov/pubmed/37242116 http://dx.doi.org/10.3390/nano13101700 |
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author | Kim, Hanul Uddin, Inayat Watanabe, Kenji Taniguchi, Takashi Whang, Dongmok Kim, Gil-Ho |
author_facet | Kim, Hanul Uddin, Inayat Watanabe, Kenji Taniguchi, Takashi Whang, Dongmok Kim, Gil-Ho |
author_sort | Kim, Hanul |
collection | PubMed |
description | A two-dimensional (2D) atomic crystalline transition metal dichalcogenides has shown immense features, aiming for future nanoelectronic devices comparable to conventional silicon (Si). 2D molybdenum ditelluride (MoTe(2)) has a small bandgap, appears close to that of Si, and is more favorable than other typical 2D semiconductors. In this study, we demonstrate laser-induced p-type doping in a selective region of n-type semiconducting MoTe(2) field effect transistors (FET) with an advance in using the hexagonal boron nitride as passivation layer from protecting the structure phase change from laser doping. A single nanoflake MoTe(2)-based FET, exhibiting initial n-type and converting to p-type in clear four-step doping, changing charge transport behavior in a selective surface region by laser doping. The device shows high electron mobility of about 23.4 cm(2)V(−1)s(−1) in an intrinsic n-type channel and hole mobility of about 0.61 cm(2)V(−1)s(−1) with a high on/off ratio. The device was measured in the range of temperature 77–300 K to observe the consistency of the MoTe(2)-based FET in intrinsic and laser-dopped region. In addition, we measured the device as a complementary metal–oxide–semiconductor (CMOS) inverter by switching the charge-carrier polarity of the MoTe(2) FET. This fabrication process of selective laser doping can potentially be used for larger-scale MoTe(2) CMOS circuit applications. |
format | Online Article Text |
id | pubmed-10222443 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-102224432023-05-28 Conversion of Charge Carrier Polarity in MoTe(2) Field Effect Transistor via Laser Doping Kim, Hanul Uddin, Inayat Watanabe, Kenji Taniguchi, Takashi Whang, Dongmok Kim, Gil-Ho Nanomaterials (Basel) Communication A two-dimensional (2D) atomic crystalline transition metal dichalcogenides has shown immense features, aiming for future nanoelectronic devices comparable to conventional silicon (Si). 2D molybdenum ditelluride (MoTe(2)) has a small bandgap, appears close to that of Si, and is more favorable than other typical 2D semiconductors. In this study, we demonstrate laser-induced p-type doping in a selective region of n-type semiconducting MoTe(2) field effect transistors (FET) with an advance in using the hexagonal boron nitride as passivation layer from protecting the structure phase change from laser doping. A single nanoflake MoTe(2)-based FET, exhibiting initial n-type and converting to p-type in clear four-step doping, changing charge transport behavior in a selective surface region by laser doping. The device shows high electron mobility of about 23.4 cm(2)V(−1)s(−1) in an intrinsic n-type channel and hole mobility of about 0.61 cm(2)V(−1)s(−1) with a high on/off ratio. The device was measured in the range of temperature 77–300 K to observe the consistency of the MoTe(2)-based FET in intrinsic and laser-dopped region. In addition, we measured the device as a complementary metal–oxide–semiconductor (CMOS) inverter by switching the charge-carrier polarity of the MoTe(2) FET. This fabrication process of selective laser doping can potentially be used for larger-scale MoTe(2) CMOS circuit applications. MDPI 2023-05-22 /pmc/articles/PMC10222443/ /pubmed/37242116 http://dx.doi.org/10.3390/nano13101700 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Communication Kim, Hanul Uddin, Inayat Watanabe, Kenji Taniguchi, Takashi Whang, Dongmok Kim, Gil-Ho Conversion of Charge Carrier Polarity in MoTe(2) Field Effect Transistor via Laser Doping |
title | Conversion of Charge Carrier Polarity in MoTe(2) Field Effect Transistor via Laser Doping |
title_full | Conversion of Charge Carrier Polarity in MoTe(2) Field Effect Transistor via Laser Doping |
title_fullStr | Conversion of Charge Carrier Polarity in MoTe(2) Field Effect Transistor via Laser Doping |
title_full_unstemmed | Conversion of Charge Carrier Polarity in MoTe(2) Field Effect Transistor via Laser Doping |
title_short | Conversion of Charge Carrier Polarity in MoTe(2) Field Effect Transistor via Laser Doping |
title_sort | conversion of charge carrier polarity in mote(2) field effect transistor via laser doping |
topic | Communication |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10222443/ https://www.ncbi.nlm.nih.gov/pubmed/37242116 http://dx.doi.org/10.3390/nano13101700 |
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