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Low frequency transconductance and output resistance dispersion of epitaxial graphene nanoribbon-based field effect transistors

机译:外延石墨烯纳米型场效应晶体管的低频跨导和输出电阻分散

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Graphene-based devices have recently attracted strong attention due to very promising features such as two-dimensional material properties and high carrier mobility [1]. Significant effort has been placed on studies of high frequency characteristics of graphene transistors [2, 3] and first low-frequency noise studies have been reported [4]. However the low-frequency transconductance and output resistance dispersion of graphene FETs are less understood. These play a major role in determining the device performance and are the subject of the studies reported in this paper. The channel or the ungated region of the device is usually responsible for such effects. The Graphene Nano Ribbon Field Effect Transistors (GNRFETs) reported here have been fabricated using an array of parallel graphene nano ribbons, described in [2]. The devices were dual gate FETs fabricated with coplanar access structure for RF characterization. Ni/Au (50/300 nm) was used for source and drain contacts and the GNR array was defined by e-beam lithography. To achieve accurate ribbon width control, hydrogen silsesquioxane (HSQ) was used as mask material. The excess of graphene surface was then etched by O2 RIE. After removing HSQ, the Al2O3 gate oxide was obtained by oxidation of a thin aluminium layer (about 2nm) in two steps leading to a final thickness of ∼ 5 nm. Finally, the top gate (Lg=150 nm) was realized using Ni/Au 50/300nm. The photograph of the final device is shown in Fig. 1.
机译:由于非常有希望的特征,如二维材料特性和高载流子移动性,最近,基于石墨烯的装置最近引起了强烈的关注[1]。已经对石墨烯晶体管的高频特性进行了重大努力[2,3],并报道了第一种低频噪声研究[4]。然而,石墨烯FET的低频跨导和输出电阻分散较少被理解。这些在确定设备性能方面发挥了重要作用,并且是本文报告的研究主题。该设备的通道或未通道区域通常对这种效果负责。这里报道的石墨烯纳米带场效应晶体管(GNRFET)使用并联石墨烯纳米带阵列制造了[2]。该器件是具有用于RF表征的共面访问结构的双栅FET。 Ni / Au(50/300nm)用于源极和漏极触点,通过电子束光刻限定GNR阵列。为了实现精确的色带宽度控制,氢倍半硅氧烷(HSQ)用作掩模材料。然后通过O 2 RIE蚀刻过量的石墨烯表面。除去HSQ后,通过在两个步骤中氧化薄铝层(约2nm)而导致〜5nm的最终厚度的薄铝层(约2nm)获得Al 2 栅极氧化物。最后,使用Ni / Au 50 / 300nm实现顶部门(L G = 150nm)。最终装置的照片如图1所示。1。

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