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混合金属纳米阵列中的等离子体激元激发

Plasmon Excitations in Mixed Metallic Nanoarrays.

作者信息

Conley Kevin M, Nayyar Neha, Rossi Tuomas P, Kuisma Mikael, Turkowski Volodymyr, Puska Martti J, Rahman Talat S

机构信息

Department of Applied Physics, COMP Centre of Excellence , Aalto University School of Science , P.O. Box 11100, FI-00076 Aalto , Finland.

Department of Applied Physics, QTF Centre of Excellence , Aalto University School of Science , P.O. Box 11100, FI-00076 Aalto , Finland.

出版信息

ACS Nano. 2019 May 28;13(5):5344-5355. doi: 10.1021/acsnano.8b09826. Epub 2019 Apr 17.

Abstract

Features of the surface plasmon from macroscopic materials emerge in molecular systems, but differentiating collective excitations from single-particle excitations in molecular systems remains elusive. The rich interactions between single-particle electron-hole and collective electron excitations produce phenomena related to the chemical physics aspects within the atomic array. We study the plasmonic properties of atomic arrays of noble (Au, Ag, and Cu) and transition-metal (Pd, Pt) homonuclear chains using time-dependent density functional theory and their Kohn-Sham transition contributions. The response to the electromagnetic radiation is related to both the geometry-dependent confinement of sp-valence electrons and the energy position of d-electrons in the different atomic species and the hybridization between d and sp electrons. It is possible to tune the position of the plasmon resonance, split it into several peaks, and eventually achieve broadband absorption of radiation. Arrays of mixed noble and transition-metal chains may have strongly attenuated plasmonic behavior. The collective nature of the excitations is ascertained using their Kohn-Sham transition contributions. To manipulate the plasmonic response and achieve the desired properties for broad applications, it is vital to understand the origins of these phenomena in atomic chains and their arrays.

摘要

宏观材料中的表面等离子体激元特征出现在分子系统中,但区分分子系统中的集体激发和单粒子激发仍然很困难。单粒子电子 - 空穴与集体电子激发之间丰富的相互作用产生了与原子阵列内化学物理方面相关的现象。我们使用含时密度泛函理论及其Kohn - Sham跃迁贡献来研究贵金属(金、银和铜)和过渡金属(钯、铂)同核链原子阵列的等离子体激元性质。对电磁辐射的响应既与sp价电子的几何相关限制有关,也与不同原子种类中d电子的能量位置以及d电子与sp电子之间的杂化有关。可以调节等离子体激元共振的位置,将其分裂成几个峰,并最终实现辐射的宽带吸收。混合贵金属和过渡金属链的阵列可能具有强烈衰减的等离子体激元行为。利用它们的Kohn - Sham跃迁贡献来确定激发的集体性质。为了操纵等离子体激元响应并实现广泛应用所需的特性,了解原子链及其阵列中这些现象的起源至关重要。

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