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Compact Super Electron-Donor to Monolayer MoS 2
The surface functionalization of two-dimensional (2D) materials with organic electron donors (OEDs) is a powerful tool to modulate the electronic properties of the material. Here we report a novel molecular dopant, Me-OED, that demonstrates record-breaking molecular doping to MoS , achieving a carri...
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Published in: | Nano letters 2022-06, Vol.22 (11), p.4501-4508 |
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container_end_page | 4508 |
container_issue | 11 |
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container_title | Nano letters |
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creator | Reed-Lingenfelter, Serrae N Chen, Yifeng Yarali, Milad Charboneau, David J Curley, Julia B Hynek, David J Wang, Mengjing Williams, Natalie L Hazari, Nilay Quek, Su Ying Cha, Judy J |
description | The surface functionalization of two-dimensional (2D) materials with organic electron donors (OEDs) is a powerful tool to modulate the electronic properties of the material. Here we report a novel molecular dopant, Me-OED, that demonstrates record-breaking molecular doping to MoS
, achieving a carrier density of 1.10 ± 0.37 × 10
cm
at optimal functionalization conditions; the achieved carrier density is much higher than those by other OEDs such as benzyl viologen and an OED based on 4,4'-bipyridine. This impressive doping power is attributed to the compact size of Me-OED, which leads to high surface coverage on MoS
. To confirm, we study
Bu-OED, which has an identical reduction potential to Me-OED but is significantly larger. Using field-effect transistor measurements and spectroscopic characterization, we estimate the doping powers of Me- and
Bu-OED are 0.22-0.44 and 0.11 electrons per molecule, respectively, in good agreement with calculations. Our results demonstrate that the small size of Me-OED is critical to maximizing the surface coverage and molecular interactions with MoS
, enabling us to achieve unprecedented doping of MoS
. |
doi_str_mv | 10.1021/acs.nanolett.2c01167 |
format | article |
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, achieving a carrier density of 1.10 ± 0.37 × 10
cm
at optimal functionalization conditions; the achieved carrier density is much higher than those by other OEDs such as benzyl viologen and an OED based on 4,4'-bipyridine. This impressive doping power is attributed to the compact size of Me-OED, which leads to high surface coverage on MoS
. To confirm, we study
Bu-OED, which has an identical reduction potential to Me-OED but is significantly larger. Using field-effect transistor measurements and spectroscopic characterization, we estimate the doping powers of Me- and
Bu-OED are 0.22-0.44 and 0.11 electrons per molecule, respectively, in good agreement with calculations. Our results demonstrate that the small size of Me-OED is critical to maximizing the surface coverage and molecular interactions with MoS
, enabling us to achieve unprecedented doping of MoS
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, achieving a carrier density of 1.10 ± 0.37 × 10
cm
at optimal functionalization conditions; the achieved carrier density is much higher than those by other OEDs such as benzyl viologen and an OED based on 4,4'-bipyridine. This impressive doping power is attributed to the compact size of Me-OED, which leads to high surface coverage on MoS
. To confirm, we study
Bu-OED, which has an identical reduction potential to Me-OED but is significantly larger. Using field-effect transistor measurements and spectroscopic characterization, we estimate the doping powers of Me- and
Bu-OED are 0.22-0.44 and 0.11 electrons per molecule, respectively, in good agreement with calculations. Our results demonstrate that the small size of Me-OED is critical to maximizing the surface coverage and molecular interactions with MoS
, enabling us to achieve unprecedented doping of MoS
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, achieving a carrier density of 1.10 ± 0.37 × 10
cm
at optimal functionalization conditions; the achieved carrier density is much higher than those by other OEDs such as benzyl viologen and an OED based on 4,4'-bipyridine. This impressive doping power is attributed to the compact size of Me-OED, which leads to high surface coverage on MoS
. To confirm, we study
Bu-OED, which has an identical reduction potential to Me-OED but is significantly larger. Using field-effect transistor measurements and spectroscopic characterization, we estimate the doping powers of Me- and
Bu-OED are 0.22-0.44 and 0.11 electrons per molecule, respectively, in good agreement with calculations. Our results demonstrate that the small size of Me-OED is critical to maximizing the surface coverage and molecular interactions with MoS
, enabling us to achieve unprecedented doping of MoS
.</abstract><cop>United States</cop><pmid>35609247</pmid><doi>10.1021/acs.nanolett.2c01167</doi><tpages>8</tpages><orcidid>https://orcid.org/0000-0003-0112-7030</orcidid><orcidid>https://orcid.org/0000-0003-4216-8242</orcidid><orcidid>https://orcid.org/0000-0003-4223-2953</orcidid><orcidid>https://orcid.org/0000-0002-6346-2814</orcidid><orcidid>https://orcid.org/0000-0003-1195-4515</orcidid><orcidid>https://orcid.org/0000-0001-8337-198X</orcidid></addata></record> |
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title | Compact Super Electron-Donor to Monolayer MoS 2 |
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