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Plasmons at the LaAlO_3/SrTiO_3 interface and in the graphene-LaAlO_3/SrTiO_3 double layer

机译:等离子在LaAlO_3 / SrTiO_3界面和石墨烯-LaAlO_3 / SrTiO_3双层中

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摘要

We study plasmon modes of the two-dimensional electron gas residing at the interface of band insulators LaAlO_3 and SrTiO_3 (LAO/STO) and the plasmon excitations of graphene-LAO/STO double layer as well. Considering the electron-electron interaction within random phase approximation, we calculate the plasmon dispersions of both systems numerically and in the long-wavelength limit analytical expressions for collective modes are found. One optical mode and two (three) acoustic modes are predicted for the LAO/STO (graphene- LAO/STO) system where only the uppermost acoustic mode of both systems can emerge above the electron-hole continuum depending on the characteristics of each system. In the case of LAO/STO interface, thanks to the spatial separation between t_(2g) orbitals, the upper acoustic mode might be undamped at the long-wavelength limit depending on the exact value of the dielectric constant of SrTi03. Same as other double layer systems, the interlayer distance for the graphene-LAO/STO system plays a crucial role in damping the upper acoustic mode. Faster damping of all plasmon modes of the present double layer system in comparison with the ones with conventional two-dimensional electron gas instead of t2g electron gas is also found due to heavier effective masses of the gas and also stronger interlayer Coulomb interaction.
机译:我们研究了位于带绝缘子LaAlO_3和SrTiO_3(LAO / STO)界面上的二维电子气的等离子体激元模式,以及石墨烯-LAO / STO双层的等离子体激元激发。考虑到随机相近似下的电子-电子相互作用,我们通过数值计算了两个系统的等离激元色散,并在长波长范围内找到了集体模式的解析表达式。对于LAO / STO(石墨烯-LAO / STO)系统,预测了一种光学模式和两种(三种)声学模式,其中,根据每个系统的特性,两个系统中只有最高声学模式才能出现在电子-空穴连续体上方。在LAO / STO界面的情况下,由于t_(2g)轨道之间存在空间间隔,取决于SrTiO3介电常数的确切值,上声模可能在长波长极限处没有衰减。与其他双层系统相同,石墨烯-LAO / STO系统的层间距离在阻尼上声模中起着至关重要的作用。与常规的二维电子气代替t 2g电子气相比,本双层系统的所有等离激元模式的阻尼也更快,这是因为该气体的有效质量较重并且层间库仑相互作用更强。

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  • 来源
    《Physical review》 |2017年第16期|165419.1-165419.13|共13页
  • 作者

    A. Faridi; Reza Asgari;

  • 作者单位

    Department of Physics, Sharif University of Technology, Tehran, Iran,School of Physics, Institute for Research in Fundamental Sciences (IPM), Tehran 19395-5531, Iran;

    School of Physics, Institute for Research in Fundamental Sciences (IPM), Tehran 19395-5531, Iran,School of Nano Science, Institute for Research in Fundamental Sciences (IPM), Tehran 19395-5531, Iran;

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