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首页> 外文期刊>Carbon: An International Journal Sponsored by the American Carbon Society >Transfer-matrix simulations of electronic transport in single-wall and multi-wall carbon nanotubes
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Transfer-matrix simulations of electronic transport in single-wall and multi-wall carbon nanotubes

机译:单壁和多壁碳纳米管中电子传输的传递矩阵模拟

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We present simulations of electronic transport in single-wall and multi-wall carbon nanotubes, which are placed between two metallic contacts. We consider situations where the electrons first encounter a singe-wall nanotube (corresponding to either the inner or the outer shell of the (10, 10)@(15,15)@(20,20) and (10, 10)@(20, 10)@(20,20) nanotubes), before encountering the multi-wall structures. The role of this two-step procedure is to enforce the electrons to enter a single shell of the multi-wall nanotubes, and we study how from that point they get redistributed amongst the other tubes. Because of reflections at the metallic contacts, the conductance of finite armchair nanotubes is found to depend on the length of the tubes, with values that alternate between three separate functions. Regarding the transport in multi-wall nanotubes, it is found that the electrons keep essentially propagating in the shell in which they are initially injected, with transfers to the other tubes hardly exceeding one percent of the whole current. In the case where the three tubes are conducting, these transfers are already completed after four nanometers. The conductance and repartition of the current present then oscillations, which are traced to the band structure of the nanotube. The transfers between the shells and the amplitude of these oscillations are significantly reduced when the intermediate tube is semiconducting. (C) 2004 Elsevier Ltd. All rights reserved.
机译:我们提出了单壁和多壁碳纳米管中电子传输的模拟,它们位于两个金属触点之间。我们考虑电子首先遇到单壁纳米管的情况(对应于(10,10)@(15,15)@(20,20)和(10,10)@( 20,10)@(20,20)纳米管),然后再遇到多壁结构。此两步过程的作用是强制电子进入多壁纳米管的单个壳中,并且我们研究如何从此角度将电子重新分配到其他管中。由于金属接触处的反射,发现有限的扶手椅状纳米管的电导率取决于管的长度,其值在三个独立的函数之间交替。关于在多壁纳米管中的传输,发现电子基本上在最初注入它们的壳中保持传播,到其他管的传输几乎不超过整个电流的百分之一。在三个管导通的情况下,这些转移已在四纳米后完成。电流的传导和重新分配随后发生振荡,这可追溯到纳米管的能带结构。当中间管为半导体时,壳之间的传递和这些振荡的幅度会大大降低。 (C)2004 Elsevier Ltd.保留所有权利。

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