Department of Chemistry, National University of Singapore, 3 Science Drive 3, Singapore 117543.
J Am Chem Soc. 2011 Oct 5;133(39):15397-411. doi: 10.1021/ja201223n. Epub 2011 Sep 14.
This paper describes the performance of junctions based on self-assembled monolayers (SAMs) as the functional element of a half-wave rectifier (a simple circuit that converts, or rectifies, an alternating current (AC) signal to a direct current (DC) signal). Junctions with SAMs of 11-(ferrocenyl)-1-undecanethiol or 11-(biferrocenyl)-1-undecanethiol on ultraflat, template-stripped Ag (Ag(TS)) bottom electrodes, and contacted by top electrodes of eutectic indium-gallium (EGaIn), rectified AC signals, while similar junctions based on SAMs of 1-undecanethiol-SAMs lacking the ferrocenyl terminal group-did not. SAMs in these AC circuits (operating at 50 Hz) remain stable over a larger window of applied bias than in DC circuits. AC measurements, therefore, can investigate charge transport in SAM-based junctions at magnitudes of bias inaccessible to DC measurements. For junctions with SAMs of alkanethiols, combining the results from AC and DC measurements identifies two regimes of bias with different mechanisms of charge transport: (i) low bias (|V| < 1.3 V), at which direct tunneling dominates, and (ii) high bias (|V| > 1.3 V), at which Fowler-Nordheim (FN) tunneling dominates. For junctions with SAMs terminated by Fc moieties, the transition to FN tunneling occurs at |V| ≈ 2.0 V. Furthermore, at sufficient forward bias (V > 0.5 V), hopping makes a significant contribution to charge transport and occurs in series with direct tunneling (V ≲ 2.0 V) until FN tunneling activates (V ≳ 2.0 V). Thus, for Fc-terminated SAMs at forward bias, three regimes are apparent: (i) direct tunneling (V = 0-0.5 V), (ii) hopping plus direct tunneling (V ≈ 0.5-2.0 V), and (iii) FN tunneling (V ≳ 2.0 V). Since hopping does not occur at reverse bias, only two regimes are present over the measured range of reverse bias. This difference in the mechanisms of charge transport at forward and reverse bias for junctions with Fc moieties resulted in large rectification ratios (R > 100) and enabled half-wave rectification.
本文描述了基于自组装单分子层 (SAM) 的结作为半波整流器 (一种将交流 (AC) 信号转换或整流为直流 (DC) 信号的简单电路) 的功能元件的性能。具有 11-(二茂铁基)-1-十一硫醇或 11-(双二茂铁基)-1-十一硫醇 SAM 的结在超平整、模板剥离的 Ag (Ag(TS)) 底电极上,并由共晶铟镓 (EGaIn) 的顶电极接触,对 AC 信号进行整流,而类似的基于缺乏二茂铁末端基团的 1-十一硫醇 SAM 的结则没有。在交流电路中 (工作频率为 50 Hz),SAMs 比在直流电路中保持更大的偏置窗口稳定。因此,交流测量可以在直流测量无法达到的偏置幅度下研究基于 SAM 的结中的电荷输运。对于具有烷硫醇 SAM 的结,将交流和直流测量的结果结合起来,可以确定两种具有不同电荷输运机制的偏置范围:(i) 低偏置 (|V| < 1.3 V),此时主要是直接隧道;(ii) 高偏置 (|V| > 1.3 V),此时主要是福勒-诺德海姆 (FN) 隧道。对于由 Fc 部分端接的 SAMs 的结,向 FN 隧道的转变发生在 |V| ≈ 2.0 V。此外,在足够的正向偏置 (V > 0.5 V) 下,跳跃对电荷输运有显著贡献,并且与直接隧道 (V ≲ 2.0 V) 串联,直到 FN 隧道激活 (V ≳ 2.0 V)。因此,对于正向偏置的 Fc 端接的 SAMs,有三个明显的区域:(i) 直接隧道 (V = 0-0.5 V),(ii) 跳跃加直接隧道 (V ≈ 0.5-2.0 V),和 (iii) FN 隧道 (V ≳ 2.0 V)。由于在反向偏置时不会发生跳跃,因此在测量的反向偏置范围内仅存在两个区域。这种具有 Fc 部分的结在正向和反向偏置下的电荷输运机制的差异导致了大的整流比 (R > 100),并实现了半波整流。