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穿透电子探测金属纳米颗粒中受限体等离子体和贝内特等离子体的原子尺度表征

Atomistic Characterization of Confined Bulk and Bennett Plasmons in Metallic Nanoparticles as Probed by Penetrating Electrons.

作者信息

Candelas Bruno, Urbieta Mattin, Babaze Antton, Ogando Eduardo, Borisov Andrei G, Zabala Nerea, Aizpurua Javier

机构信息

Materials Physics Center, CSIC-UPV/EHU, Manuel de Lardizabal 5, 20018 Donostia, Spain.

Donostia International Physics Center, Manuel de Lardizabal 4, 20018 Donostia, Spain.

出版信息

J Phys Chem Lett. 2025 Mar 27;16(12):2965-2971. doi: 10.1021/acs.jpclett.5c00157. Epub 2025 Mar 14.

Abstract

Despite the experimental observation of confined bulk plasmons (CBPs) in metallic nanostructures using electron energy-loss spectroscopy (EELS), there is still a limited theoretical understanding of their resonance structure when they are excited by penetrating electron beams. In this work, we use atomistic time-dependent density functional theory (TDDFT) to perform a first-principles study of the excitation of CBPs induced by swift electrons. Our quantum approach offers a parameter-free framework for the calculation of the EEL spectra of metallic nanoparticles with atomistic resolution, while jellium TDDFT and classical hydrodynamic calculations allow us to unravel the rich spectral pattern associated with CBPs. Additionally, the excitation of high-energy surface resonances characterized by an induced dipole moment across the nanoparticle surface, known as Bennett modes, is also explored. This study represents a significant step forward in the exploration of plasmonic signatures in the EELS of metallic nanoparticles.

摘要

尽管利用电子能量损失谱(EELS)在金属纳米结构中通过实验观察到了受限体等离子体激元(CBP),但对于它们在被穿透电子束激发时的共振结构,理论理解仍然有限。在这项工作中,我们使用原子尺度的含时密度泛函理论(TDDFT)对快速电子诱导的CBP激发进行了第一性原理研究。我们的量子方法为计算具有原子分辨率的金属纳米颗粒的EEL光谱提供了一个无参数框架,而凝胶模型TDDFT和经典流体动力学计算使我们能够揭示与CBP相关的丰富光谱模式。此外,还探索了以纳米颗粒表面诱导偶极矩为特征的高能表面共振激发,即贝内特模式。这项研究在探索金属纳米颗粒EELS中的等离子体特征方面向前迈出了重要一步。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0acd/11956129/b0a5955ad7fc/jz5c00157_0001.jpg

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