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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Self-modulation doping effect in the high-mobility layered semiconductor Bi_2O_2Se
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Self-modulation doping effect in the high-mobility layered semiconductor Bi_2O_2Se

机译:高迁移率层状半导体Bi_2O_2Se中的自调制掺杂效应

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Recently, an air-stable layered semiconductor Bi_2O_2Se was discovered to exhibit an ultrahigh mobility in transistors fabricated with its thin layers. In this work, we explored the mechanism that induces the high mobility and distinguishes Bi_2O_2Se from other semiconductors. We found that the electron donor states lie above the lowest conduction band. Thus, electrons gel spontaneously ionized from donor sites (e.g.. Se vacancies) without involving the thermal activation, different from the donor ionization in conventional semiconductors. Consequently, the resistance decreases as reducing the temperature as observed in our measurement, which is similar to a metal but contrasts to a usual semiconductor. Furthermore, the electron conduction channels locate spatially away from ionized donor defects (Se vacancies) in different van der Waals layers. Such a spatial separation can strongly suppress the scattering caused by donor sites and subsequently increase the electron mobility, especially at the low temperature. We call this high-mobility mechanism self-modulation doping, i.e., the modulation doping spontaneously happening in a single-phase material without requiring a heterojunction. Our work paves a way to design high-mobility semiconductors with layered materials.
机译:近来,发现在其薄层制成的晶体管中,空气稳定的层状半导体Bi_2O_2Se具有超高迁移率。在这项工作中,我们探索了诱导高迁移率并将Bi_2O_2Se与其他半导体区分开的机制。我们发现电子给体状态位于最低导带之上。因此,与常规半导体中的施主电离不同,电子自施主位点(例如,Se空位)自发地凝胶化而没有涉及热活化。因此,正如我们在测量中观察到的那样,电阻随着温度的降低而降低,这与金属相似,但与常规半导体相反。此外,电子传导通道在空间上远离不同范德华层中的电离施主缺陷(Se空位)。这样的空间分离可以强烈地抑制由施主位点引起的散射,并且随后增加电子迁移率,特别是在低温下。我们将这种高迁移率机制称为自调制掺杂,即在单相材料中自发发生调制掺杂而无需异质结。我们的工作为采用分层材料设计高迁移率半导体铺平了道路。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2018年第24期|241203.1-241203.5|共5页
  • 作者单位

    Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 7610001, Israel;

    Center for Nanochemistrx, Beijing Sciences and Engineering Centre for Nanocarhons, College of Chemistry and Molecular Engineering, Peking University, Beijing 100871, China;

    Center for Nanochemistrx, Beijing Sciences and Engineering Centre for Nanocarhons, College of Chemistry and Molecular Engineering, Peking University, Beijing 100871, China;

    Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 7610001, Israel;

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