Sub-10 nm epitaxial graphene nanoribbon FETs

K. Tahy, W. Hwang, J. Tedesco, R. Myers-Ward, P. Campbell, C. Eddy, D. Gaskill, H. Xing, A. Seabaugh, D. Jena
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引用次数: 3

Abstract

Graphene is being investigated as a promising candidate for electronic devices. For digital electronic devices, a substantial bandgap is necessary. It is possible to open a bandgap in graphene by quantum confinement of the carriers in patterned graphene nanoribbons (GNRs); GNRs with width W nm have a bandgap Eg∼1.3/W eV [1]. This implies that sub-10 nm wide ribbons can enable room-temperature operation of GNRs as traditional semiconductors, but with ultimate vertical scaling, and still take advantage of high current drives. To date, GNRs have been fabricated from exfoliated graphene [2] and operated by back gates, or nanometer scale ribbons produced by ‘explosive’ methods [3] that are neither controlled nor reproducible. These methods are not suitable for large-area device fabrication. In this work, we report lithographically patterned GNRs on epitaxial graphene on SiC substrates. Specifically, we show the first top-gated GNR field-effect transistors (FETs) on epi-graphene substrates that exhibit the opening of a substantial energy bandgap (exceeding ∼0.15 eV at a ribbon width of 10 nm), respectable carrier mobility (700 – 800 cm2/Vs), high current modulation (10∶1 at 300 K), and high current carrying capacity (0.3 mA/µm at VDS = 1 V) at the same time. Both single GNR and GNR array devices are reported.
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亚10nm外延石墨烯纳米带场效应管
石墨烯作为一种有前途的电子器件候选者正在被研究。对于数字电子设备来说,需要一个大的带隙。在石墨烯纳米带(GNRs)中,通过量子约束载流子可以在石墨烯中打开带隙;宽度为W nm的gnr具有Eg ~ 1.3/W eV的带隙[1]。这意味着低于10纳米宽的带可以使gnr像传统半导体一样在室温下工作,但具有最终的垂直缩放,并且仍然可以利用大电流驱动。迄今为止,gnr是由剥离的石墨烯[2]制成的,并通过后门或由“爆炸”方法[3]生产的纳米级带进行操作,这些方法既不可控也不可复制。这些方法不适用于大面积器件的制造。在这项工作中,我们报道了在SiC衬底上外延石墨烯上的光刻图案化gnr。具体来说,我们展示了第一个顶门控GNR场效应晶体管(fet)在epi-石墨烯衬底上,同时表现出大量能量带隙的打开(在10 nm的带宽下超过~ 0.15 eV),可观的载流子迁移率(700 - 800 cm2/Vs),高电流调制(10∶1在300 K)和高电流承载能力(0.3 mA/µm在VDS = 1 V)。报道了单GNR和GNR阵列器件。
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