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首页> 外文期刊>Physica status solidi, B. Basic research >Non-equilibrium Green function implementation of boundary conditions for full band simulations of substrate-nanowire structures
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Non-equilibrium Green function implementation of boundary conditions for full band simulations of substrate-nanowire structures

机译:基板-纳米线结构全频带模拟的边界条件的非平衡格林函数实现

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The density of states of a nanowire exhibits peaks at energies in which the individual transverse modes begin to propagate. Under ideal conditions these modes are eigenstates solely determined by the cross sectional size and shape of the nanowire. However, for realistic nanowires, which are grown on semiconductor substrates, the density of states of the subsrate-nanowire structure is dependent on the distance from the nanowire endpoints. Near the substrate, the density of states is is nonzero far below the energy corresponding to the first eigenstate of the ideal nanowire. This initial increase in the density of states occurs at energies near the conduction and valence band edges of the semiconductor substrate on which the nanowire is grown. Away from the substrate, the density of states begins to acquire ideal nanowire characteristics. In the present work this effect is captured by imposing boundary conditions, with properties of bulk material, at the nanowire base. The calculations utilize a first neighbor sp(3)s*d(5) orbital basis within the non-equilibrium Green function formalism. (C) 2003 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim. [References: 7]
机译:纳米线的状态密度在各个横向模式开始传播的能量处显示出峰值。在理想条件下,这些模式是本征态,仅由纳米线的横截面尺寸和形状决定。然而,对于在半导体衬底上生长的现实的纳米线,基底-纳米线结构的状态密度取决于与纳米线端点的距离。在衬底附近,态密度为非零,远低于与理想纳米线的第一个本征态相对应的能量。状态密度的这种初始增加发生在在其上生长纳米线的半导体衬底的导带和价带边缘附近的能量处。离开衬底,状态密度开始获得理想的纳米线特性。在本工作中,通过在纳米线基底上施加具有块状材料特性的边界条件来捕获这种效果。该计算利用非平衡格林函数形式主义内的第一近邻sp(3)s * d(5)轨道基础。 (C)2003 WILEY-VCH Verlag GmbH&Co.KGaA,Weinheim。 [参考:7]

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