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构象依赖性通过分子断键结的电传导

Conformation-dependent conductance through a molecular break junction.

机构信息

Institute for Solid State Theory, Department of Physics, University of Münster, Wilhelm-Klemm Str. 10, 48149, Münster, Germany,

出版信息

J Mol Model. 2013 Oct;19(10):4173-80. doi: 10.1007/s00894-013-1794-z. Epub 2013 Feb 27.

Abstract

Ab initio molecular dynamics simulations have been performed of a gold-1,4-benzenedithiol (BDT)-gold nanojunction under mechanical stress. For three different pulling rates between 10 and 40 m s(-1), it is found that the nanowire always ruptures between the second and third Au atom from the thiol sulfur. Larger rupture forces and longer extensions are required at higher pulling rates and vice versa. The electrical conductance was calculated along a pulling trajectory using the DFT-NEGF method to study the effect of thermal and stress-induced structural changes on the electrical transport properties. While the mechanically induced stretching of the junction is seen to lower the time-averaged conductance, thermal conformational changes are capable of altering the conductance by one order of magnitude. No single geometric quantity could be identified as the main contributor to the conductance fluctuations. Small modulations, however, can be explained in terms of C=C double bond vibrations in the BDT molecule. The dependence of the conductance on different geometric variables has further been investigated systematically by performing constrained geometry optimizations along a number of angle and dihedral coordinates. The largest changes in the conductance are observed when the Au-S-C angle and the Au-S-C-C dihedral are simultaneously constrained.

摘要

采用从头算分子动力学模拟方法研究了金-1,4-苯二硫醇(BDT)-金纳结在机械应力下的情况。在 10 到 40 m s(-1) 的三个不同的拉伸速率下,发现纳线总是在硫原子的第二个和第三个 Au 原子之间断裂。较高的拉伸速率需要更大的断裂力和更长的延伸,反之亦然。通过使用 DFT-NEGF 方法沿着拉伸轨迹计算电导率,以研究热和应力诱导的结构变化对电输运性质的影响。虽然机械诱导的结拉伸被认为会降低时间平均电导率,但热构象变化能够使电导率改变一个数量级。没有一个单一的几何量可以被确定为电导波动的主要贡献者。然而,小的调制可以用 BDT 分子中的 C=C 双键振动来解释。通过沿着许多角度和二面角坐标进行约束几何优化,进一步系统地研究了电导对不同几何变量的依赖性。当 Au-S-C 角和 Au-S-C-C 二面角同时受到约束时,电导的变化最大。

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