Gong J M, Khan M S S, Da B, Yoshikawa H, Tanuma S, Ding Z J
Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China.
Center for Basic Research on Materials, National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan.
Phys Chem Chem Phys. 2023 Aug 9;25(31):20917-20932. doi: 10.1039/d3cp01413d.
Core-shell nanoparticles (NPs) are active research areas for their unique properties and wide applications. By changing the elemental composition in the core and shell, a series of core-shell NPs with specific functions can be obtained, where the sizes of the core and shell also influence the properties. X-ray photoelectron spectroscopy (XPS) is useful in this context as a means of quantitatively analyzing such NPs. The empirical formula proposed by Shard [, 2012, (31), 16806-16813] for calculating the shell thickness of the spherical core-shell NPs has been verified by Powell [, 2016, (39), 22730-22738] through a simulation of XPS with Simulation of Electron Spectra for Surface Analysis (SESSA) software. However, real core-shell NPs are not necessarily ideal spheres; such NPs can have rich shapes and uneven thicknesses. This work aims to extend the Shard formula to non-ideal core-shell NPs. We have used a Monte Carlo simulation method to study the XPS signal variation with the shell thickness for several modeled non-spherical shapes of core-shell NPs including some complex geometric structures which are numerically constructed with finite-element triangular meshes. Five types of non-spherical shapes, egg, ellipsoid, rod, rough-surface, and star shapes, are considered, while the size parameters are varied over a wide range. The equivalent radius and equivalent thickness are defined to characterize the average size of the nanoparticles for the use of the Shard formula. We have thus derived an extended Shard formula for the specific core-shell NPs, with which the relative error between the predicted shell thickness and the real thickness can be reduced to less than 10%.
核壳纳米粒子(NPs)因其独特的性质和广泛的应用而成为活跃的研究领域。通过改变核和壳中的元素组成,可以获得一系列具有特定功能的核壳纳米粒子,其中核和壳的尺寸也会影响其性质。在这种情况下,X射线光电子能谱(XPS)作为定量分析此类纳米粒子的一种手段很有用。Shard [2012年,(31),16806 - 16813]提出的用于计算球形核壳纳米粒子壳层厚度的经验公式已被Powell [2016年,(39),22730 - 22738]通过使用表面分析电子能谱模拟(SESSA)软件进行XPS模拟得到验证。然而,实际的核壳纳米粒子不一定是理想的球体;此类纳米粒子可以具有丰富的形状和不均匀的厚度。这项工作旨在将Shard公式扩展到非理想核壳纳米粒子。我们使用蒙特卡罗模拟方法研究了几种建模的非球形核壳纳米粒子(包括一些用有限元三角形网格数值构建的复杂几何结构)的XPS信号随壳层厚度的变化。考虑了五种非球形形状,即卵形、椭球形、棒形、粗糙表面形和星形,同时尺寸参数在很宽的范围内变化。定义了等效半径和等效厚度以表征纳米粒子的平均尺寸,以便使用Shard公式。因此,我们为特定的核壳纳米粒子推导了一个扩展的Shard公式,利用该公式预测的壳层厚度与实际厚度之间的相对误差可降低到小于10%。