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电场驱动金纳米颗粒单层在硅基底上的自组装

Electric Field-Driven Self-Assembly of Gold Nanoparticle Monolayers on Silicon Substrates.

作者信息

Deader Firdous Ahmad, Abbas Yawar, Qurashi Ahsanulhaq, Al-Qutayri Mahmoud, Chan Vincent, Rezeq Moh'd

机构信息

Department of Physics, Khalifa University, Abu Dhabi 127788, United Arab Emirates.

System on Chip Lab, Khalifa University, Abu Dhabi 127788, United Arab Emirates.

出版信息

Langmuir. 2023 Nov 7;39(44):15766-15772. doi: 10.1021/acs.langmuir.3c02351. Epub 2023 Oct 25.

DOI:10.1021/acs.langmuir.3c02351
PMID:37879624
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10634370/
Abstract

Nanoparticles (NPs) bridge the gap between bulk materials and their equivalent molecular/atomic counterparts. The physical, optical, and electronic properties of individual NPs alter with the changes in their surrounding environment at the nanoscale. Similarly, the characteristics of thin films of NPs depend on their lateral and volumetric densities. Thus, attaining single monolayers of these NPs would play a vital role in the improved characteristics of semiconductor devices such as nanosensors, field effect transistors, and energy harvesting devices. Developing nanosensors, for instance, requires precise methods to fabricate a monolayer of NPs on selected substrates for sensing and other applications. Herein, we developed a physical fabrication method to form a monolayer of NPs on a planar silicon surface by creating an electric field of intensity 5.71 × 10 V/m between parallel plates of a capacitor, by applying a DC voltage. The physics of monolayer formation caused by an externally applied electric field on the gold NPs (Au-NPs) of size 20 nm in diameter and possesses a zeta potential of -250 to -290 mV, is further analyzed with the help of the finite element simulation. The enhanced electric field, in the order of 10 V/m, around the Au-NPs indicates a high surface charge density on the NPs, which results in a high electric force per unit area that guides them to settle uniformly on the surface of the silicon substrate.

摘要

纳米颗粒(NPs)弥合了块状材料与其等效分子/原子对应物之间的差距。单个纳米颗粒的物理、光学和电子特性会随着纳米尺度下其周围环境的变化而改变。同样,纳米颗粒薄膜的特性取决于它们的横向和体积密度。因此,获得这些纳米颗粒的单分子层对于改善诸如纳米传感器、场效应晶体管和能量收集装置等半导体器件的特性将起到至关重要的作用。例如,开发纳米传感器需要精确的方法在选定的基板上制造纳米颗粒的单分子层以用于传感和其他应用。在此,我们开发了一种物理制造方法,通过在电容器的平行板之间施加直流电压,创建强度为5.71×10 V/m的电场,在平面硅表面形成纳米颗粒的单分子层。借助有限元模拟进一步分析了由外部施加的电场在直径为20 nm且zeta电位为 -250至 -290 mV的金纳米颗粒(Au-NPs)上引起的单分子层形成的物理过程。金纳米颗粒周围增强的电场(约为10 V/m)表明纳米颗粒上具有高表面电荷密度,这导致每单位面积的高电力,引导它们均匀地沉积在硅基板表面。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/bc85384ad3ed/la3c02351_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/45c56e89087a/la3c02351_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/35466b17438f/la3c02351_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/d8a9a80815ca/la3c02351_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/e6fd1f7a57eb/la3c02351_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/2ba107946721/la3c02351_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/bc85384ad3ed/la3c02351_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/45c56e89087a/la3c02351_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/35466b17438f/la3c02351_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/d8a9a80815ca/la3c02351_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/e6fd1f7a57eb/la3c02351_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/2ba107946721/la3c02351_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/27d6/10634370/bc85384ad3ed/la3c02351_0006.jpg

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