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通过直流磁控溅射和惰性气体冷凝制备银纳米团簇:结构、开尔文探针力显微镜及光学性质研究

Ag Nanocluster Production through DC Magnetron Sputtering and Inert Gas Condensation: A Study of Structural, Kelvin Probe Force Microscopy, and Optical Properties.

作者信息

Musa Ishaq, Qamhieh Naser, Mahmoud Saleh T

机构信息

Department of Physics, Palestine Technical University-Kadoorie, Tulkarem P.O. Box 7, Palestine.

Department of Physics, UAE University, Al-Ain P.O. Box 15551, United Arab Emirates.

出版信息

Nanomaterials (Basel). 2023 Oct 13;13(20):2758. doi: 10.3390/nano13202758.

Abstract

Silver nanoclusters are valuable for a variety of applications. A combination of direct current (DC) magnetron sputtering and inert gas condensation methods, employed within an ultra-high vacuum (UHV) system, was used to generate Ag nanoclusters with an average size of 4 nm. Various analytical techniques, including Scanning Probe Microscopy (SPM), X-ray Diffraction (XRD), Kelvin Probe Force Microscopy (KPFM), UV-visible absorption, and Photoluminescence, were employed to characterize the produced Ag nanoclusters. AFM topographic imaging revealed spherical nanoparticles with sizes ranging from 3 to 6 nm, corroborating data from a quadrupole mass filter (QMF). The XRD analysis verified the simple cubic structure of the Ag nanoclusters. The surface potential was assessed using KPFM, from which the work function was calculated with a reference highly ordered pyrolytic graphite (HOPG). The UV-visible absorption spectra displayed peaks within the 350-750 nm wavelength range, with a strong absorption feature at 475 nm. Additionally, lower excitation wavelengths resulted in a sharp peak emission at 370 nm, which became weaker and broader when higher excitation wavelengths were used.

摘要

银纳米团簇在各种应用中都很有价值。在超高真空(UHV)系统中采用直流(DC)磁控溅射和惰性气体冷凝方法相结合,来生成平均尺寸为4 nm的银纳米团簇。采用了各种分析技术,包括扫描探针显微镜(SPM)、X射线衍射(XRD)、开尔文探针力显微镜(KPFM)、紫外-可见吸收和光致发光,来表征所制备的银纳米团簇。原子力显微镜(AFM)形貌成像显示尺寸范围为3至6 nm的球形纳米颗粒,这与四极质量过滤器(QMF)的数据相符。XRD分析证实了银纳米团簇的简单立方结构。使用KPFM评估表面电势,并以此为基础用参考的高度有序热解石墨(HOPG)计算功函数。紫外-可见吸收光谱在350 - 750 nm波长范围内显示出峰值,在475 nm处有强烈的吸收特征。此外,较低的激发波长会在370 nm处产生尖锐的峰值发射,而使用较高的激发波长时,该发射会变得更弱且更宽。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b53/10609199/1065a02857f4/nanomaterials-13-02758-g001.jpg

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