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...
Saved in:
Published in | IEEE electron device letters Vol. 41; no. 10; pp. 1592 - 1595 |
---|---|
Main Authors | , , , , , , , |
Format | Journal Article |
Language | English |
Published |
New York
IEEE
01.10.2020
The Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
Subjects | |
Online Access | Get full text |
Cover
Loading…
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 |