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首页> 外文期刊>Journal of Applied Physics >Spin-dependent transport properties through gapless graphene-based ferromagnet and gapped graphene-based superconductor junction
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Spin-dependent transport properties through gapless graphene-based ferromagnet and gapped graphene-based superconductor junction

机译:通过无间隙石墨烯基铁磁体和带隙石墨烯基超导体结的自旋相关输运性质

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摘要

By depositing a superconductor on gapped graphene (graphene grown on SiC substrate), the motion of quasiparticles in this superconductor is explained by the massive Dirac equation. In this paper, we study the spin dependent transport properties of graphene-based ferromagnetic/insulator/superconductor (FIS) junction and graphene-based ferromagnetic/ferromagnetic barrier/superconductor (FF_BS) junction in which only the superconducting region is deposited on the gapped graphene and the other graphene regions are gapless. We found that in the graphene-based FIS junction and in the thin barrier approximation, by opening the energy gap in the superconducting region, the charge conductance is an oscillatory function of barrier strength (X_G), despite the large Fermi energy mismatch between ferromagnetic and superconductor regions. As an important result, we analytically obtained that for the normal incident of charge carriers, this junction is not totally transparent. This means that the second characteristic of Klein tunneling is not satisfied due to the massive Dirac fermions carrying the current in the superconductor region. For the graphene-based FF_BS junction, opening the energy gap causes a phase shift as large as π/2 to appear between the peaks of charge conductance for parallel and antiparallel configuration versus x_G. Interestingly, we obtained that by increasing the energy gap in this junction, the magnetoresistance increases and by approaching the energy gap to the Fermi energy of the superconductor, it reaches its maximum value (more than -150%). This characteristic shows that this junction can be a suitable candidate for application in the graphene-based spintronics devices.
机译:通过在有间隙的石墨烯(在SiC衬底上生长的石墨烯)上沉积超导体,该超导体中的准粒子的运动可以用大量的狄拉克方程来解释。在本文中,我们研究了石墨烯基铁磁/绝缘体/超导体(FIS)结和石墨烯基铁磁/铁磁势垒/超导体(FF_BS)结的自旋依赖输运性质,其中仅超导区域沉积在有间隙的石墨烯上其他石墨烯区域无间隙。我们发现,在基于石墨烯的FIS结和薄势垒近似中,通过打开超导区域中的能隙,尽管铁磁和铁磁之间的费米能量失配较大,但电荷电导是势垒强度(X_G)的振荡函数。超导区域。作为一个重要的结果,我们通过分析得出,对于载流子的垂直入射,该结并不完全透明。这意味着由于在超导体区域中携带大量电流的狄拉克费米子,不能满足克莱因隧穿的第二个特征。对于基于石墨烯的FF_BS结,打开能隙会导致x和G平行和反平行配置的电荷电导峰值之间出现最大π/ 2的相移。有趣的是,我们获得了通过增加该结处的能隙,磁阻增加,并使能隙接近超导体的费米能,使其达到最大值(大于-150%)的方法。该特性表明,该结可以适合用于基于石墨烯的自旋电子器件中。

著录项

  • 来源
    《Journal of Applied Physics》 |2012年第1期|p.013901.1-013901.10|共10页
  • 作者单位

    Department of Physics, Faculty of Sciences, University of Shahid Chamran, Ahwaz, Iran;

    Department of Physics, Faculty of Sciences, University of Shahid Chamran, Ahwaz, Iran;

    Department of Physics, Faculty of Sciences, University of Isfahan, Hezar Jerib Avenue,Isfahan 81746-73441, Iran;

  • 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
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