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High-performance multilayer WSe2 field-effect transistors with carrier type control

机译:具有载流子类型控制的高性能多层WSe2场效应晶体管

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摘要

In this study,high-performance multilayer WSe2 field-effect transistor (FET) devices with carrier type control are demonstrated via thickness modulation and a remote oxygen plasma surface treatment.Carrier type control in multilayer WSe2 FET devices with Cr/Au contacts is initially demonstrated by modulating the WSe2 thickness.The carrier type evolves with increasing WSe2 channel thickness,being p-type,ambipolar,and n-type at thicknesses < 3,~ 4,and > 5 nm,respectively.The thickness-dependent carrier type is attributed to changes in the bandgap of WSe2 as a function of the thickness and the carrier band offsets relative to the metal contacts.Furthermore,we present a strong hole carrier doping effect via remote oxygen plasma treatment.It non-degenerately converts n-type characteristics into p-type and enhances field-effect hole mobility by three orders of magnitude.This work demonstrates progress towards the realization of high-performance multilayer WSe2 FETs with carrier type control,potentially extendable to other transition metal dichalcogenides,for future electronic and optoelectronic applications.
机译:在这项研究中,通过厚度调制和远程氧等离子体表面处理展示了具有载流子类型控制的高性能多层WSe2场效应晶体管(FET)器件。最初展示了具有Cr / Au触点的多层WSe2 FET器件的载流子类型控制。通过调节WSe2的厚度,载流子类型随WSe2沟道厚度的增加而演化,分别为厚度小于3,〜4和> 5 nm的p型,双极性和n型。 WSe2的带隙随厚度和载流子相对于金属接触的偏移而变化。此外,我们通过远程氧等离子体处理表现出强大的空穴载流子掺杂效应。它不退化地将n型特征转化为p型,并将场效应空穴迁移率提高了三个数量级。这项工作展示了在实现具有载流子类型控制的高性能多层WSe2 FET方面的进展,可能扩展到其他过渡金属二卤化物,用于未来的电子和光电应用。

著录项

  • 来源
    《纳米研究(英文版)》 |2018年第2期|722-730|共9页
  • 作者单位

    Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Bredesen Center for Interdisciplinary Research and Graduate Education, University of Tennessee, Knoxville, TN 37996, USA;

    Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

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  • 入库时间 2022-08-19 03:47:25
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