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The performance limits of hexagonal boron nitride as an insulator for scaled CMOS devices based on two-dimensional materials

机译:基于二维材料缩放CMOS器件的六边形氮化物作为绝缘体的性能限制

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摘要

Complementary metal-oxide-semiconductor (CMOS) logic circuits at their ultimate scaling limits place extreme demands on the properties of all materials involved. The requirements for semiconductors are well explored and could possibly be satisfied by a number of layered two-dimensional (2D) materials, such as transition metal dichalcogenides or black phosphorus. The requirements for gate insulators are arguably even more challenging. At present, hexagonal boron nitride (hBN) is the most common 2D insulator and is widely considered to be the most promising gate insulator in 2D material-based transistors. Here we assess the material parameters and performance limits of hBN. We compare experimental and theoretical tunnel currents through ultrathin layers (equivalent oxide thickness of less than 1 nm) of hBN and other 2D gate insulators, including the ideal case of defect-free hBN. Though its properties make hBN a candidate for many applications in 2D nanoelectronics, excessive leakage currents lead us to conclude that hBN is unlikely to be suitable for use as a gate insulator in ultrascaled CMOS devices.This Perspective assesses the performance limits of hexagonal boron nitride when used as a gate insulator in complementary metal-oxide-semiconductor (CMOS) devices based on two-dimensional materials, concluding that due to excessive leakage currents, the material is unlikely to be suitable for use in ultrascaled CMOS devices.
机译:互补金属氧化物半导体(CMOS)逻辑电路在其最终缩放限制下对所有所涉及的所有材料的性质进行极大的需求。探索半导体的要求良好,并且可以通过多种分层的二维(2D)材料,例如过渡金属二甲基化物或黑磷来满足。栅极绝缘体的要求可以说是更具挑战性的。目前,六边形氮化硼(HBN)是最常见的2D绝缘体,并且被广泛认为是基于2D材料的晶体管中最有前景的栅极绝缘体。在这里,我们评估HBN的材料参数和性能限制。我们通过HBN和其他2D栅极绝缘体的超薄层(等同氧化物厚度小于1nm)的超薄层(相当于1nm)的实验和理论隧道电流,包括无缺陷HbN的理想情况。虽然其性质使HBN成为2D纳米电子产品中许多应用的候选者,但过多的漏电流导致我们得出结论,HBN不太可能适合用作普通的CMOS器件中的栅极绝缘体。这一透视评估六边形氮化物的性能限制用作基于二维材料的互补金属 - 氧化物半导体(CMOS)器件的栅极绝缘体,得出代表性的,由于过度泄漏电流,该材料不太可能适用于丝光的CMOS器件。

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  • 来源
    《Nature Electronics》 |2021年第2期|98-108|共11页
  • 作者单位

    TU Wien Inst Microelect Vienna Austria;

    TU Wien Inst Microelect Vienna Austria|Ioffe Inst St Petersburg Russia;

    Swiss Fed Inst Technol Integrated Syst Lab Zurich Switzerland;

    TU Wien Inst Microelect Christian Doppler Lab Single Defect Spect Semicon Vienna Austria;

    TU Wien Inst Photon Vienna Austria;

    Natl Inst Mat Sci Funct Mat Res Ctr Res Ctr Funct Mat Tsukuba Ibaraki Japan;

    Natl Inst Mat Sci Int Ctr Mat Nanoarchitecton Tsukuba Ibaraki Japan;

    TU Wien Inst Photon Vienna Austria;

    TU Wien Inst Microelect Christian Doppler Lab Single Defect Spect Semicon Vienna Austria;

    King Abdullah Univ Sci & Technol KAUST Phys Sci & Engn Div Thuwal Saudi Arabia;

    Ioffe Inst St Petersburg Russia;

    Swiss Fed Inst Technol Integrated Syst Lab Zurich Switzerland;

    TU Wien Inst Microelect Vienna Austria;

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