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Top-Gated Graphene Field-Effect Transistors Using Graphene on Si (111) Wafers

机译:在Si(111)晶圆上使用石墨烯的顶栅石墨烯场效应晶体管

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In this letter, we report the first experimental demonstration of wafer-scale ambipolar field-effect transistor (FET) on Si (111) substrates by synthesizing a graphene layer on top of 3C–SiC(111)/Si(111) substrates. With lateral scaling of the source–drain distance to 1 $mu hbox{m}$ in a top-gated layout, the on-state current of 225 $muhbox{A}/muhbox{m}$ and peak transconductance of $>hbox{40} muhbox{S}/muhbox{m}$ were obtained at $hbox{Vds} = hbox{2} hbox{V}$, which is the highest performance of graphene-on-Si FETs. The peak field-effect mobilities of 285 $ hbox{cm}^{2}/hbox{Vs}$ for holes and 175 $hbox{cm}^{2}/ hbox{Vs}$ for electrons were demonstrated, which is higher than that of ultra-thin-body SOI (n, p) MOSFETs.
机译:在这封信中,我们报告了通过在3C–SiC(111)/ Si(111)衬底顶部合成石墨烯层在Si(111)衬底上进行晶圆级双极性场效应晶体管(FET)的首次实验演示。在顶部浇口布局中,源极-漏极距离的横向缩放至1 $ mu hbox {m} $,通态电流为225 $ muhbox {A} / muhbox {m} $,峰值跨导为$> hbox以$ hbox {Vds} = hbox {2} hbox {V} $的价格获得{40} muhbox {S} / muhbox {m} $,这是硅上石墨烯FET的最高性能。空穴的峰值场效应迁移率为285 $ hbox {cm} ^ {2} / hbox {Vs} $,电子的峰值场效应迁移率为175 $ hbox {cm} ^ {2} / hbox {Vs} $,较高。比超薄型SOI(n,p)MOSFET要大。

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