Ultrahigh Doping of Graphene Using Flame-Deposited MoO3

The expected high performance of graphene-based electronics is often hindered by lack of adequate doping, which causes low carrier density and large sheet resistance. Many reported graphene doping schemes also suffer from instability or incompatibility with existing semiconductor processing. Here we...

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Bibliographic Details
Published inIEEE electron device letters Vol. 41; no. 10; pp. 1592 - 1595
Main Authors Vaziri, Sam, Chen, Victoria, Cai, Lili, Jiang, Yue, Chen, Michelle E., Grady, Ryan W., Zheng, Xiaolin, Pop, Eric
Format Journal Article
LanguageEnglish
Published New York IEEE 01.10.2020
The Institute of Electrical and Electronics Engineers, Inc. (IEEE)
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Summary:The expected high performance of graphene-based electronics is often hindered by lack of adequate doping, which causes low carrier density and large sheet resistance. Many reported graphene doping schemes also suffer from instability or incompatibility with existing semiconductor processing. Here we report ultrahigh and stable <inline-formula> <tex-math notation="LaTeX">{p} </tex-math></inline-formula>-type doping up to <inline-formula> <tex-math notation="LaTeX">\sim 7\times 10 ^{13} </tex-math></inline-formula> cm −2 (<inline-formula> <tex-math notation="LaTeX">\sim 2\times 10 ^{21} </tex-math></inline-formula> cm −3 ) of monolayer graphene grown by chemical vapor deposition. This is achieved by direct polycrystalline MoO 3 growth on graphene using a rapid flame synthesis technique. With this approach, the metal-graphene contact resistance for holes is reduced to <inline-formula> <tex-math notation="LaTeX">\sim 200~\Omega \cdot \mu \text{m} </tex-math></inline-formula>. We also demonstrate that flame-deposited MoO 3 provides over <inline-formula> <tex-math notation="LaTeX">5\times </tex-math></inline-formula> higher doping of graphene, as well as superior thermal and long-term stability, compared to electron-beam deposited MoO 3 .
ISSN:0741-3106
1558-0563
DOI:10.1109/LED.2020.3018485