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Comparative analysis of Schottky barriers for heterogeneous defect domains in monolayer WS2 field-effect transistors

[Display omitted] •We investigated the Schottky barrier (SB) characteristics depending on the S vacancy (SV) and W vacancy (WV) in hexagonal WS2 field-effect transistors (FETs)•In comparison to the WV FET, the SV FET exhibited a 10 times higher doping concentration and 4 times higher Coulomb scatter...

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Published in:Applied surface science 2022-12, Vol.604, p.154600, Article 154600
Main Authors: Kim, Jungchun, An, Gwang Hwi, Bang, Seain, Park, Dong Geun, Kim, Donghyun, Jin, Seunghee, Kim, Min Jung, Lee, Hyun Seok, Lee, Jae Woo
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cited_by cdi_FETCH-LOGICAL-c221t-53c5e71b8dc8419ce958d8faabfbb4d9544944f3f9e9fd76a472b667af7db57f3
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container_title Applied surface science
container_volume 604
creator Kim, Jungchun
An, Gwang Hwi
Bang, Seain
Park, Dong Geun
Kim, Donghyun
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Kim, Min Jung
Lee, Hyun Seok
Lee, Jae Woo
description [Display omitted] •We investigated the Schottky barrier (SB) characteristics depending on the S vacancy (SV) and W vacancy (WV) in hexagonal WS2 field-effect transistors (FETs)•In comparison to the WV FET, the SV FET exhibited a 10 times higher doping concentration and 4 times higher Coulomb scattering coefficient.•The comparative SB characteristics of both FETs were investigated by Arrhenius plot for the on-current at high temperatures. A major bottleneck in the applications of two-dimensional transition metal dichalcogenides (TMDs) is the realization of ohmic contacts by overcoming the Schottky barrier (SB) at metal–semiconductor interfaces. Although the physical properties of point defects in TMDs are the key to determining the SB characteristics, the correlation between the defect types and SBs is yet to be systematically explored. Here, we investigated the SB characteristics depending on the S vacancy (SV) and W vacancy (WV) in hexagonal WS2 field-effect transistors (FETs). This was implemented by fabricating the SV and WV FETs in each domain on a single-flake monolayer. Compared to WV FET, the SV FET exhibited a 10 times higher doping concentration and 4 times higher Coulomb scattering coefficient (α) resulting in higher low-frequency noise. The comparative SB characteristics of both FETs were investigated by Arrhenius plot for the on-current at high temperatures. Below 360 K, the activation energies (Ea) of the SV and WV FETs exhibited different values of 0.071 and 0.115 eV, respectively, whereas those values are similar above 360 K because sufficient thermal energy allows for tunneling at SBs. These results help us understand the correlation between the defect type, doping level, and SB in TMD-based electronic devices.
doi_str_mv 10.1016/j.apsusc.2022.154600
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A major bottleneck in the applications of two-dimensional transition metal dichalcogenides (TMDs) is the realization of ohmic contacts by overcoming the Schottky barrier (SB) at metal–semiconductor interfaces. Although the physical properties of point defects in TMDs are the key to determining the SB characteristics, the correlation between the defect types and SBs is yet to be systematically explored. Here, we investigated the SB characteristics depending on the S vacancy (SV) and W vacancy (WV) in hexagonal WS2 field-effect transistors (FETs). This was implemented by fabricating the SV and WV FETs in each domain on a single-flake monolayer. Compared to WV FET, the SV FET exhibited a 10 times higher doping concentration and 4 times higher Coulomb scattering coefficient (α) resulting in higher low-frequency noise. The comparative SB characteristics of both FETs were investigated by Arrhenius plot for the on-current at high temperatures. Below 360 K, the activation energies (Ea) of the SV and WV FETs exhibited different values of 0.071 and 0.115 eV, respectively, whereas those values are similar above 360 K because sufficient thermal energy allows for tunneling at SBs. These results help us understand the correlation between the defect type, doping level, and SB in TMD-based electronic devices.</description><identifier>ISSN: 0169-4332</identifier><identifier>EISSN: 1873-5584</identifier><identifier>DOI: 10.1016/j.apsusc.2022.154600</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Activation energy ; Contact resistance ; Field-effect transistor ; Heterogeneous defect domains ; Hexagonal WS2 monolayer ; Low frequency noise</subject><ispartof>Applied surface science, 2022-12, Vol.604, p.154600, Article 154600</ispartof><rights>2022 Elsevier B.V.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c221t-53c5e71b8dc8419ce958d8faabfbb4d9544944f3f9e9fd76a472b667af7db57f3</citedby><cites>FETCH-LOGICAL-c221t-53c5e71b8dc8419ce958d8faabfbb4d9544944f3f9e9fd76a472b667af7db57f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Kim, Jungchun</creatorcontrib><creatorcontrib>An, Gwang Hwi</creatorcontrib><creatorcontrib>Bang, Seain</creatorcontrib><creatorcontrib>Park, Dong Geun</creatorcontrib><creatorcontrib>Kim, Donghyun</creatorcontrib><creatorcontrib>Jin, Seunghee</creatorcontrib><creatorcontrib>Kim, Min Jung</creatorcontrib><creatorcontrib>Lee, Hyun Seok</creatorcontrib><creatorcontrib>Lee, Jae Woo</creatorcontrib><title>Comparative analysis of Schottky barriers for heterogeneous defect domains in monolayer WS2 field-effect transistors</title><title>Applied surface science</title><description>[Display omitted] •We investigated the Schottky barrier (SB) characteristics depending on the S vacancy (SV) and W vacancy (WV) in hexagonal WS2 field-effect transistors (FETs)•In comparison to the WV FET, the SV FET exhibited a 10 times higher doping concentration and 4 times higher Coulomb scattering coefficient.•The comparative SB characteristics of both FETs were investigated by Arrhenius plot for the on-current at high temperatures. A major bottleneck in the applications of two-dimensional transition metal dichalcogenides (TMDs) is the realization of ohmic contacts by overcoming the Schottky barrier (SB) at metal–semiconductor interfaces. Although the physical properties of point defects in TMDs are the key to determining the SB characteristics, the correlation between the defect types and SBs is yet to be systematically explored. Here, we investigated the SB characteristics depending on the S vacancy (SV) and W vacancy (WV) in hexagonal WS2 field-effect transistors (FETs). This was implemented by fabricating the SV and WV FETs in each domain on a single-flake monolayer. Compared to WV FET, the SV FET exhibited a 10 times higher doping concentration and 4 times higher Coulomb scattering coefficient (α) resulting in higher low-frequency noise. The comparative SB characteristics of both FETs were investigated by Arrhenius plot for the on-current at high temperatures. Below 360 K, the activation energies (Ea) of the SV and WV FETs exhibited different values of 0.071 and 0.115 eV, respectively, whereas those values are similar above 360 K because sufficient thermal energy allows for tunneling at SBs. 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A major bottleneck in the applications of two-dimensional transition metal dichalcogenides (TMDs) is the realization of ohmic contacts by overcoming the Schottky barrier (SB) at metal–semiconductor interfaces. Although the physical properties of point defects in TMDs are the key to determining the SB characteristics, the correlation between the defect types and SBs is yet to be systematically explored. Here, we investigated the SB characteristics depending on the S vacancy (SV) and W vacancy (WV) in hexagonal WS2 field-effect transistors (FETs). This was implemented by fabricating the SV and WV FETs in each domain on a single-flake monolayer. Compared to WV FET, the SV FET exhibited a 10 times higher doping concentration and 4 times higher Coulomb scattering coefficient (α) resulting in higher low-frequency noise. The comparative SB characteristics of both FETs were investigated by Arrhenius plot for the on-current at high temperatures. Below 360 K, the activation energies (Ea) of the SV and WV FETs exhibited different values of 0.071 and 0.115 eV, respectively, whereas those values are similar above 360 K because sufficient thermal energy allows for tunneling at SBs. These results help us understand the correlation between the defect type, doping level, and SB in TMD-based electronic devices.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.apsusc.2022.154600</doi></addata></record>
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subjects Activation energy
Contact resistance
Field-effect transistor
Heterogeneous defect domains
Hexagonal WS2 monolayer
Low frequency noise
title Comparative analysis of Schottky barriers for heterogeneous defect domains in monolayer WS2 field-effect transistors
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