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Monitoring dopants by Raman scattering in an electrochemically top-gated graphene transistor
被引:3108
作者:
Das, A.
[1
,2
]
Pisana, S.
Chakraborty, B.
[1
,2
]
Piscanec, S.
Saha, S. K.
[2
]
Waghmare, U. V.
[3
]
Novoselov, K. S.
[4
]
Krishnamurthy, H. R.
[2
]
Geim, A. K.
[4
]
Ferrari, A. C.
[1
]
Sood, A. K.
[2
]
机构:
[1] Univ Cambridge, Dept Engn, Cambridge CB3 0FA, England
[2] Indian Inst Sci, Dept Phys, Bangalore 560012, Karnataka, India
[3] Jawaharlal Nehru Ctr Adv Sci Res, Theoret Sci Unit, Bangalore 560064, Karnataka, India
[4] Univ Manchester, Dept Phys & Astron, Manchester M13 9PL, Lancs, England
关键词:
D O I:
10.1038/nnano.2008.67
中图分类号:
TB3 [工程材料学];
学科分类号:
0805 ;
080502 ;
摘要:
The recent discovery of graphene(1-3) has led to many advances in two-dimensional physics and devices(4,5). The graphene devices fabricated so far have relied on SiO2 back gating(1-3). Electrochemical top gating is widely used for polymer transistors(6,7), and has also been successfully applied to carbon nanotubes(8,9). Here we demonstrate a top-gated graphene transistor that is able to reach doping levels of up to 5x10(13) cm(-2), which is much higher than those previously reported. Such high doping levels are possible because the nanometre-thick Debye layer(8,10) in the solid polymer electrolyte gate provides a much higher gate capacitance than the commonly used SiO2 back gate, which is usually about 300 nm thick(11). In situ Raman measurements monitor the doping. The G peak stiffens and sharpens for both electron and hole doping, but the 2D peak shows a different response to holes and electrons. The ratio of the intensities of the G and 2D peaks shows a strong dependence on doping, making it a sensitive parameter to monitor the doping.
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页码:210 / 215
页数:6
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