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Enhancing the graphene photocurrent using surface plasmons and a p-n junction

机译:使用表面等离子体和P-N结增强石墨烯光电流

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摘要

Based on the enhancement conditions of optical heating and an electrical junction, graphene photodetectors can be categorized into four cases, each represented by a row. In all plots, the horizontal axes denote the spatial coordinate x, and the vertical axes are denoted by their respective column headers. The T(x) column illustrates the electron temperature profile owing to laser illumination, and the dT/dx column is obtained by taking the spatial derivative of T(x). s(x) represents the spatial distribution of the Seebeck coefficient, and the s(x)∙(dT/dx) column is obtained by taking the product of the s(x) and dT/dx columns. The PTE current is calculated by integrating the s(x)∙(dT/dx) function, i.e., adding the areas of the shaded regions, with red (blue) denoting the positive (negative) contribution to the PTE current
机译:基于光学加热和电结的增强条件,石墨烯光电探测器可以分为四个情况,每个情况下由一行表示。在所有图中,水平轴表示空间坐标x,并且垂直轴由它们各自的列标题表示。 T(x)列由于激光照射而示出了电子温度曲线,并且通过采用t(x)的空间衍生物获得DT / DX柱。 S(x)表示塞贝克系数的空间分布,并且通过占S(x)和dt / dx列的乘积来获得S(x)∙(dt / dx)列。通过集成S(x)∙(dt / dx)函数,即添加着阴影区域的区域,用红色(蓝色)来计算PTE电流,表示对PTE电流的正(负)贡献

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