Electrochemically Top Gated Graphene: Monitoring Dopants by Raman Scattering
| dc.creator | Das, A. | |
| dc.creator | Pisana, S. | |
| dc.creator | Piscanec, S. | |
| dc.creator | Chakraborty, B. | |
| dc.creator | Saha, S. K. | |
| dc.creator | Waghmare, U. V. | |
| dc.creator | Yiang, R. | |
| dc.creator | Krishnamurhthy, H. R. | |
| dc.creator | Geim, A. K. | |
| dc.creator | Ferrari, A. C. | |
| dc.creator | Sood, A. K. | |
| dc.date | 2007-09-08 | |
| dc.date.accessioned | 2026-07-07T09:56:46Z | |
| dc.date.available | 2026-07-07T09:56:46Z | |
| dc.description | We demonstrate electrochemical top gating of graphene by using a solid polymer electrolyte. This allows to reach much higher electron and hole doping than standard back gating. In-situ Raman measurements monitor the doping. The G peak stiffens and sharpens for both electron and hole doping, while the 2D peak shows a different response to holes and electrons. Its position increases for hole doping, while it softens for high electron doping. The variation of G peak position is a signature of the non-adiabatic Kohn anomaly at $Γ$. On the other hand, for visible excitation, the variation of the 2D peak position is ruled by charge transfer. The intensity ratio of G and 2D peaks shows a strong dependence on doping, making it a sensitive parameter to monitor charges. | |
| dc.description | 7 pages, 8 figures | |
| dc.identifier | https://arxiv.org/abs/0709.1174 | |
| dc.identifier | http://arxiv.org/abs/0709.1174 | |
| dc.identifier | Nature Nanotechnology 3, 210 - 215 (01 Apr 2008) | |
| dc.identifier | doi:10.1038/nnano.2008.67 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/167094 | |
| dc.subject | Materials Science | |
| dc.title | Electrochemically Top Gated Graphene: Monitoring Dopants by Raman Scattering | |
| dc.type | text |