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First principles calculation of field emission from nanostructures using time-dependent density functional theory: A simplified approach

机译:使用时变密度泛函理论计算纳米结构场发射的第一原理:一种简化方法

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We introduce a new simplified method for computing the electron field emission current in short carbon nanotubes and graphene sheets using ab-initio computation in slab-periodic simulation cells. The evolution of the wave functions using Time-Dependent Density Functional Theory is computed by utilizing the CrankNicholson propagator and using the Octopus code (Castro et al., 2006 [1]), where we skip the wave function relaxation step elaborated by Han et al. (2002) [2], and apply a norm-conserving wave propagation method instead of the norm-nonconserving seventh-order Taylor Expansion method used by Araidai et al. (2004) [3]. Our method is mainly geared towards reducing the time it takes to compute the wave function propagation and enhancing the calculation precision. We found that in pristine carbon nanotubes, the emitted charge tends to emerge mostly from electrons that are concentrated at the nanotube tip region. The charge beam concentrates into specific channel structures, showing the utility of carbon nanotubes in precision emission applications.
机译:我们引入了一种新的简化方法,用于在平板周期模拟单元中使用从头计算来计算短碳纳米管和石墨烯片中的电子场发射电流。利用时变密度泛函理论,通过利用CrankNicholson传播子并使用章鱼码来计算波动函数的演化(Castro等,2006 [1]),在此我们跳过了Han等人阐述的波动函数松弛步骤。 。 (2002年)[2],并应用保范波传播方法,而不是Araidai等人使用的不守范七阶泰勒展开法。 (2004)[3]。我们的方法主要旨在减少计算波函数传播所需的时间并提高计算精度。我们发现,在原始的碳纳米管中,发射的电荷往往主要来自集中在纳米管尖端区域的电子。电荷束集中在特定的通道结构中,显示出碳纳米管在精密发射应用中的效用。

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