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A local resonance mechanism for thermal rectification in pristine/branched graphene nanoribbon junctions

机译:原始/支化石墨烯纳米带结中热整流的局部共振机制

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摘要

Using non-equilibrium molecular dynamics simulations, we investigate thermal rectification (TR) in pristine/branched graphene nanoribbon (GNR) junctions. The results indicate that the TR ratio of such junctions can reach 470% under small temperature bias, which has distinct superiority over asymmetric GNR and many other junctions. Moreover, the TR ratio decreases rapidly as the applied temperature bias increases. It seems to be against common sense that the TR ratio generally increases with temperature bias. Phonon spectra analyses reveal that the observed phenomena stem from the local resonance of longitudinal phonons in branched GNR region under negative temperature bias. Furthermore, the influence of ambient temperature, system length, branch number, and defect density is studied to obtain the optimum conditions for TR. This work extends local resonance mechanism to GNR for thermal signal manipulation. Published by AIP Publishing.
机译:使用非平衡分子动力学模拟,我们研究了原始/支化石墨烯纳米带(GNR)结中的热精馏(TR)。结果表明,在较小的温度偏置下,此类结的TR比率可达到470%,这比不对称GNR和许多其他结具有明显的优势。此外,随着施加的温度偏差增加,TR比迅速减小。 TR比通常随温度偏置而增加似乎与常识相反。声子波谱分析表明,观察到的现象源于负温度偏置下分支的GNR区中纵向声子的局部共振。此外,研究了环境温度,系统长度,分支数和缺陷密度的影响,以获得TR的最佳条件。这项工作将局部共振机制扩展到GNR以进行热信号操纵。由AIP Publishing发布。

著录项

  • 来源
    《Applied Physics Letters》 |2018年第12期|121906.1-121906.5|共5页
  • 作者单位

    Univ South China, Sch Math & Phys, Hengyang 421001, Peoples R China;

    Cent S Univ, Coll Chem & Chem Engn, Changsha 410083, Hunan, Peoples R China;

    Hunan Inst Technol, Dept Math & Phys, Hengyang 421002, Peoples R China;

    Hunan Inst Technol, Dept Math & Phys, Hengyang 421002, Peoples R China;

    Hunan Inst Technol, Dept Math & Phys, Hengyang 421002, Peoples R China;

    Hunan Univ, Sch Phys & Elect, Dept Appl Phys, Changsha 410082, Hunan, Peoples R China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-18 03:13:56

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